Plate Girder

74
PLATE GIRDER 1 By: Arif Memon (Assistant Professor) Civil Engineering Department, Laxmi Institute of e!"nology, #arigam (C"artere$ Engineer , AMIE) (BE Civil, M%e!" #tru!ture)

description

Plate girder design presentation

Transcript of Plate Girder

Page 1: Plate Girder

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PLATE GIRDER

1

By Arif Memon(Assistant Professor)

Civil Engineering DepartmentLaxmi Institute of enology

arigam(Cartere$ Engineer AMIE)(BE Civil Me truture)

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A girder is a fexural member which isrequired to carry heavy loads orelatively log sas

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Plate girders are tyically used as logsa foor girders i buildigs as bridgegirders ad as crae girders i idustrialstructures$

ommoly term girder reampers to a fexuralcrosssectio made u oamp a umber oampelemets$

They are geerally cosiderably deeertha the deeest rolled sectios adusually have webs thier tha rolled

sectios$

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oder late girders are ormallyampabricated by weldig together twofages ad a web late$

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

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riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

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Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

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C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

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oditio ampor (eam Lateral tability

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Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

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V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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Defnton of 1eamp n Pamptc Moent Ccte

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87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

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PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

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bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

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Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

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$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

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34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

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3ATgtR A33ETIG LATERAL TA(ILIT

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upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

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6eb rilig

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bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

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GEERAL gtIDERATIgt

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DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

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IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

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IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

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The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

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gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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(amp F(L+ $Camp

(amp F(L+ $Camp

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(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

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i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

7182019 Plate Girder

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 2: Plate Girder

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2

A girder is a fexural member which isrequired to carry heavy loads orelatively log sas

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3

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11

Plate girders are tyically used as logsa foor girders i buildigs as bridgegirders ad as crae girders i idustrialstructures$

ommoly term girder reampers to a fexuralcrosssectio made u oamp a umber oampelemets$

They are geerally cosiderably deeertha the deeest rolled sectios adusually have webs thier tha rolled

sectios$

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12

oder late girders are ormallyampabricated by weldig together twofages ad a web late$

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

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7182019 Plate Girder

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

7182019 Plate Girder

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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7182019 Plate Girder

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

7182019 Plate Girder

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

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V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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Defnton of 1eamp n Pamptc Moent Ccte

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87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

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Plate girders are tyically used as logsa foor girders i buildigs as bridgegirders ad as crae girders i idustrialstructures$

ommoly term girder reampers to a fexuralcrosssectio made u oamp a umber oampelemets$

They are geerally cosiderably deeertha the deeest rolled sectios adusually have webs thier tha rolled

sectios$

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12

oder late girders are ormallyampabricated by weldig together twofages ad a web late$

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

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V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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Defnton of 1eamp n Pamptc Moent Ccte

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87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

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34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

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Plate girders are tyically used as logsa foor girders i buildigs as bridgegirders ad as crae girders i idustrialstructures$

ommoly term girder reampers to a fexuralcrosssectio made u oamp a umber oampelemets$

They are geerally cosiderably deeertha the deeest rolled sectios adusually have webs thier tha rolled

sectios$

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oder late girders are ormallyampabricated by weldig together twofages ad a web late$

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

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V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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Defnton of 1eamp n Pamptc Moent Ccte

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87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

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34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 5: Plate Girder

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11

Plate girders are tyically used as logsa foor girders i buildigs as bridgegirders ad as crae girders i idustrialstructures$

ommoly term girder reampers to a fexuralcrosssectio made u oamp a umber oampelemets$

They are geerally cosiderably deeertha the deeest rolled sectios adusually have webs thier tha rolled

sectios$

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12

oder late girders are ormallyampabricated by weldig together twofages ad a web late$

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

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V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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Defnton of 1eamp n Pamptc Moent Ccte

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87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

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11

Plate girders are tyically used as logsa foor girders i buildigs as bridgegirders ad as crae girders i idustrialstructures$

ommoly term girder reampers to a fexuralcrosssectio made u oamp a umber oampelemets$

They are geerally cosiderably deeertha the deeest rolled sectios adusually have webs thier tha rolled

sectios$

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12

oder late girders are ormallyampabricated by weldig together twofages ad a web late$

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

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V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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Defnton of 1eamp n Pamptc Moent Ccte

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87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

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34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 7: Plate Girder

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Plate girders are tyically used as logsa foor girders i buildigs as bridgegirders ad as crae girders i idustrialstructures$

ommoly term girder reampers to a fexuralcrosssectio made u oamp a umber oampelemets$

They are geerally cosiderably deeertha the deeest rolled sectios adusually have webs thier tha rolled

sectios$

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12

oder late girders are ormallyampabricated by weldig together twofages ad a web late$

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

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V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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Defnton of 1eamp n Pamptc Moent Ccte

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87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 8: Plate Girder

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11

Plate girders are tyically used as logsa foor girders i buildigs as bridgegirders ad as crae girders i idustrialstructures$

ommoly term girder reampers to a fexuralcrosssectio made u oamp a umber oampelemets$

They are geerally cosiderably deeertha the deeest rolled sectios adusually have webs thier tha rolled

sectios$

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12

oder late girders are ormallyampabricated by weldig together twofages ad a web late$

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

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87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

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34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 9: Plate Girder

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10

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Plate girders are tyically used as logsa foor girders i buildigs as bridgegirders ad as crae girders i idustrialstructures$

ommoly term girder reampers to a fexuralcrosssectio made u oamp a umber oampelemets$

They are geerally cosiderably deeertha the deeest rolled sectios adusually have webs thier tha rolled

sectios$

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12

oder late girders are ormallyampabricated by weldig together twofages ad a web late$

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

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7182019 Plate Girder

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

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87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 10: Plate Girder

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Plate girders are tyically used as logsa foor girders i buildigs as bridgegirders ad as crae girders i idustrialstructures$

ommoly term girder reampers to a fexuralcrosssectio made u oamp a umber oampelemets$

They are geerally cosiderably deeertha the deeest rolled sectios adusually have webs thier tha rolled

sectios$

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12

oder late girders are ormallyampabricated by weldig together twofages ad a web late$

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

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7182019 Plate Girder

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

7182019 Plate Girder

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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7182019 Plate Girder

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 11: Plate Girder

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11

Plate girders are tyically used as logsa foor girders i buildigs as bridgegirders ad as crae girders i idustrialstructures$

ommoly term girder reampers to a fexuralcrosssectio made u oamp a umber oampelemets$

They are geerally cosiderably deeertha the deeest rolled sectios adusually have webs thier tha rolled

sectios$

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12

oder late girders are ormallyampabricated by weldig together twofages ad a web late$

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

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16

7182019 Plate Girder

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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19

7182019 Plate Girder

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

7182019 Plate Girder

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 12: Plate Girder

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12

oder late girders are ormallyampabricated by weldig together twofages ad a web late$

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

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16

7182019 Plate Girder

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

7182019 Plate Girder

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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19

7182019 Plate Girder

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

7182019 Plate Girder

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

7182019 Plate Girder

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

7182019 Plate Girder

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

7182019 Plate Girder

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

7182019 Plate Girder

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

7182019 Plate Girder

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

7182019 Plate Girder

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

7182019 Plate Girder

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

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i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 13: Plate Girder

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(ecause late girders areampabricated searately each maybe desiged idividually to resist

the alied actios usigroortios that esure low selampweight ad high load resistace$

7182019 Plate Girder

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

7182019 Plate Girder

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16

7182019 Plate Girder

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

7182019 Plate Girder

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

7182019 Plate Girder

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19

7182019 Plate Girder

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

7182019 Plate Girder

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

7182019 Plate Girder

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

7182019 Plate Girder

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

7182019 Plate Girder

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

7182019 Plate Girder

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

7182019 Plate Girder

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

7182019 Plate Girder

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

7182019 Plate Girder

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

7182019 Plate Girder

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

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i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 14: Plate Girder

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There is also cosiderable scoe amporvariatio oamp crosssectio i thelogitudial directio$ A desiger may

choose to reduce the fage thic)essor breadth+ i a oe oamp low aliedmomet$

Equally i a oe oamp high shear the

desiger might choose to thic)e theweb late$

hages i -ectio

7182019 Plate Girder

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

7182019 Plate Girder

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16

7182019 Plate Girder

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

7182019 Plate Girder

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

7182019 Plate Girder

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19

7182019 Plate Girder

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

7182019 Plate Girder

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

7182019 Plate Girder

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

7182019 Plate Girder

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

7182019 Plate Girder

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

7182019 Plate Girder

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

7182019 Plate Girder

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

7182019 Plate Girder

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

7182019 Plate Girder

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

7182019 Plate Girder

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

7182019 Plate Girder

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

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i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 15: Plate Girder

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Alteratively higher grade steel mightbe emloyed ampor oes oamp high alied

momet ad shear while stadardgrade would be used elsewhere$ ocalled hybrid girders with di0eretstregth material i the fages ad the

web o0er aother ossible meas oampmore closely matchig resistace torequiremets$

hages i aterial

7182019 Plate Girder

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16

7182019 Plate Girder

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

7182019 Plate Girder

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

7182019 Plate Girder

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19

7182019 Plate Girder

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

7182019 Plate Girder

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

7182019 Plate Girder

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

7182019 Plate Girder

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

7182019 Plate Girder

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

7182019 Plate Girder

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

7182019 Plate Girder

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

7182019 Plate Girder

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

7182019 Plate Girder

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

7182019 Plate Girder

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

7182019 Plate Girder

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 16: Plate Girder

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16

7182019 Plate Girder

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

7182019 Plate Girder

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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19

7182019 Plate Girder

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

7182019 Plate Girder

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

7182019 Plate Girder

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

7182019 Plate Girder

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

7182019 Plate Girder

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

7182019 Plate Girder

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

7182019 Plate Girder

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

7182019 Plate Girder

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

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i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 17: Plate Girder

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Ay crosssectio oamp a late girder isormally sub1ected to a combiatio oampshear amporce ad bedig momet$

The rimary ampuctio oamp the to adbottom fage lates oamp the girder is toresist the axial comressive ad tesileamporces arisig amprom the alied bedig

momet$ The rimary ampuctio oamp the web late is

to resist the alied shear amporce$

7182019 Plate Girder

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

7182019 Plate Girder

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19

7182019 Plate Girder

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

7182019 Plate Girder

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

7182019 Plate Girder

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

7182019 Plate Girder

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

7182019 Plate Girder

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

7182019 Plate Girder

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

7182019 Plate Girder

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

7182019 Plate Girder

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

7182019 Plate Girder

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

7182019 Plate Girder

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 18: Plate Girder

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Plate girders are ormally desiged to

suort heavy loads over log sas isituatios where it is ecessary to roducea e2ciet desig by rovidig girders oamphigh stregth to weight ratio$

To roduce the lowest axial fage amporce ampora give bedig momet the web deth d+must be made as large as ossible$ Toreduce the selamp weight the web thic)ess

tw+ must be reduced to a miimum$ As a cosequece i may istaces the

web late is oamp sleder roortios ad isthereampore roe to buc)lig at relatively low

values oamp alied shear$

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19

7182019 Plate Girder

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

7182019 Plate Girder

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

7182019 Plate Girder

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

7182019 Plate Girder

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

7182019 Plate Girder

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 19: Plate Girder

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19

7182019 Plate Girder

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

7182019 Plate Girder

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 20: Plate Girder

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3or e2ciet desig it is usual to choosea relatively dee girder thusmiimiig the required area oamp fagesampor a give alied momet sd$

This obviously etails a dee webwhose area will be miimied byreducig its thic)ess to the miimumrequired to carry the alied shear 4sd$

uch a web may be quite sleder i$e$ ahigh d5tw ratio+ ad may be roe to

local buc)lig ad shear buc)lig$

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 21: Plate Girder

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6eb buc)lig does ot determie theultimate stregth oamp a late girder$

Plate elemets do ot collase whethey buc)le7 they ca ossess a

substatial ostbuc)lig reserve oampresistace$

3or a e2ciet desig ay calculatiorelatig to the ultimate limit stateshould ta)e the ostbuc)lig actioito accout$

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 22: Plate Girder

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Desig riteria

22

riteria ampor desig oamp late girder maybe based o

Elastic bedbuc)lig stregth

Elastic shearbuc)lig stregth

Postbedbuc)lig stregth

Postshearbuc)ligTesio8eld+stregth

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 23: Plate Girder

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I 9lt= ectio 9Desig oamp memberssub1ected to bedig

23

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

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i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 24: Plate Girder

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24

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

81 General

82 Design Strength in Bending (Flexure)

821 Laterally Supported Beam

822 Laterally Unsupported Beams

8 eti$e Length o ompression Flanges

8amp Shear

8 Stiened e +anels

81 nd +anels design

82 nd +anels designed using ension ield ation

8 -nhor ores

8 Design o Beams and +late Girders ith Solid es

81 0inimum e hiness

82 Setional +roperties

8 Flanges Cont

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

7182019 Plate Girder

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 25: Plate Girder

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25

SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING

8 Stiener Design

81 General

82 Design o 3ntermediate rans$erse e Stieners

8 Load arrying stieners

8amp Bearing Stieners

8 Design o Load arrying Stieners

8 Design o Bearing Stieners

8 Design o Diagonal Stieners

88 Design o ension Stieners

84 orsional Stieners

815 onnetion to e o Load arrying and Bearing Stieners

811 onnetion to Flanges 812 6ollo Setions

88 Box Girders

84 +urlins and sheeting rails (girts)

815 Bending in a 7on+rinipal +lane

7182019 Plate Girder

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

7182019 Plate Girder

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

7182019 Plate Girder

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

7182019 Plate Girder

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 26: Plate Girder

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REPgtE gt3 (EA Tgt 4ERTIAL LgtADIG

26

Plastic hinge formation

Lateral deection and twist

Local buckling of

i) Flange in compression

ii) Web due to sheariii) Web in compression due to

concentrated loads

Local failure by

i) Yield of web by shear

ii) Crushing of web

iii) Buckling of thin anges

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

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ELEET gt3 PLATE GIRDER

57

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 27: Plate Girder

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27

LOCAL BUCKLING AND SECTION CLASSIFICATION

OPEN AND CLOSED SECTIONS

Strength of coreon e$er een on ampenerne rto

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Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

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i0

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 28: Plate Girder

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28

Locamp $(c)ampng of Coreon Me$er

LOCAL BUCKLING

Be coreon fampnge $(c)ampe ampocampamp+

F$rcte n coampfore ecton rone to ampocamp $(c)ampng

Locamp $(c)ampng g-e torton of c $(t nee not ampe to coampampe

7182019 Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

7182019 Plate Girder

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

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72

W(B PampPampamp

otatios

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6eb Proortioig

7182019 Plate Girder

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 29: Plate Girder

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29

LOCAL FLANGE BUCKLING - STEEL W SECTION BEAM LOA

DED AT CENTER ( UNIERSIT OF OUSTON - $amp$amp

S)) B)+ T) - 94N $amp L$+ - RMIT Uamp) B)

+ C$)$amp(360

7182019 Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

7182019 Plate Girder

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

7182019 Plate Girder

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6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 30: Plate Girder

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30

L

Benng Moent Dgr

Pamptc hnge

M p

Coampampe echn

Pamptc hnge

M p

Forton of Coampampe Mechn n Fe Be

Benng Moent Dgr

BASIC CONCEPTS OF PLASTIC T0EOR1

Frt +eamp oent M+Pamptc oent M

She fctor S 2 MM+

Rotton Cct+ 34 t M+ 3$4 M+ 5 M5M3c4 t M

Pamptfcton of Croecton (ner Benng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3174

31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3274

LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

7182019 Plate Girder

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

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i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 31: Plate Girder

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31

SECTION CLASSIFICATION

M

Rottonφ

M+

φ+ φ (

Sampener

Secoct

Coct

Pamptc

Secton Campfcton $e on MoentRotton Chrctertc

LAI3IATIgt

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

7182019 Plate Girder

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4074

40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

7182019 Plate Girder

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

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i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

7182019 Plate Girder

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6eb Proortioig

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 32: Plate Girder

7182019 Plate Girder

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LAI3IATIgtgt3 Rgt

ETIgt

32

C$-)$amp +) +) + + $+)-$+ $ )amp) +$amp $ lt) $$$amp

$ lt) $-)$amp + +amp $+ )$amp +amp

+lt)) lt) = $+ +amp ++ lt )-

$+ +amp )amp) )$amp + gt) =gt) $ $ $+

gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)

+=+) $+ +amp ++ = gt) )=) $ +$

lt) $gt $ $+ gt=amp

+) )))amp $ + $-)$amp + gt=) $+ =) $ $))

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

7182019 Plate Girder

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

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39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

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40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

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7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

7182019 Plate Girder

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6eb Proortioig

7182019 Plate Girder

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 33: Plate Girder

7182019 Plate Girder

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33

+) )))amp $ + $ )$amp + gt=) $+ =) $ $))

)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt

amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp

=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+

3711 Wlt)amp + +amp+ =) lt) )gt) lt+

gt) ++gt) $ $amp + ltamp) lt =)amp

$+$amp ++ (= lt$= $+ gt=amp $

)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)

gt)$) $+$amp $ lt) +=) )lt+amp

3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+

gt) ++gt) $ ))$amp lt) ) ) =amp)

$)$amp lt$= $+ gt=amp

372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp

+) )amp) + $$

a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3574

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3674

T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3874

38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3974

39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4074

40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4174

41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 34: Plate Girder

7182019 Plate Girder

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34

a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)

lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +

)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp

lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800

b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $

)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $

+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)

)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)

lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2

c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp

$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $

)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp

lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2

d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp

gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp

lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2

Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt

$$amp lt) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp

)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $

lt) )-$+ )$amp

7182019 Plate Girder

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3774

oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3874

38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3974

39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4074

40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

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LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

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IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

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LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

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49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

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64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

7182019 Plate Girder

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6eb Proortioig

7182019 Plate Girder

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 35: Plate Girder

7182019 Plate Girder

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7182019 Plate Girder

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T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

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oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

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38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3974

39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4074

40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

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41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4674

IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

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47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

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3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

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gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

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6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

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ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

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gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

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61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

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Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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T ti0

7182019 Plate Girder

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Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

7182019 Plate Girder

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6eb Proortioig

7182019 Plate Girder

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6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 36: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3674

T+e of Eampeent T+e ofSecton Camp of Secton

Pamptc 3 64Coct

3 74Secoct 3 84

O(ttn eampeent of

coreon fampnge

Roampampe $t le $t le 6lt= $t le 6=gt

9eampe $t le 8 $t le $t le 6

Internamp eampeent of

coreon fampnge

$enng $t le 7 $t le = $t le 7

Aamp co not ampc$ampe $t le 7

9e$ NA t

etht le 8lt t le 6lt= t le 67

Angampe $enng

Aamp

co

Crc(ampr t($e th

o(ter eter D

Dt le 7 Dt le 7 Dt le 88 7

T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent

y f

250=ε

$tle

$tle

6lt=

$tle

6=gt

not ampc$ampe $t le 6=gt

3$4t le 7=

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3774

oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3874

38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3974

39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4074

40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4174

41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4274

42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4374

43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4474

(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4674

IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4774

47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

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Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 37: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3774

oditio ampor (eam Lateral tability

37

Laterally upported Beam The desig bedig stregth oamp beams

adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered

by the yield stress

Laterally nsupported Beams

6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted

beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3874

38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3974

39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4074

40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4174

41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4274

42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4374

43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4474

(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4674

IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4774

47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 38: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3874

38

L+)+ =$) gt)+

L+)+ =amp=$) gt)+

LUSAS L+)+ T$$amp+ B=amp

$ B) gt)+(360

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3974

39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4074

40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4174

41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4274

42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4374

43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4474

(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4674

IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4774

47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 39: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 3974

39

Degn Strength n Benng 3Fampe(re4

The fctore egn oent M t n+ ecton n $e (e to

eternamp cton hampamp tf+

876 Lterampamp+ S(orte Be

T+e 6 Secton th toc)+ e$

d t w le gtε

The egn $enng trength go-erne $+ amptc trength M d

hampamp $e fo(n tho(t Sher Intercton for ampo her ce

rereente $+

5lt V d

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4074

40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4174

41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4274

42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4374

43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4474

(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4674

IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4774

47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 40: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4074

40

V exceeds $V d

Md B Mdv

M dv= design bending strength under high

shear as defined in section 9

876 Degn Benng Strength (ner 0gh Sher

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4174

41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4274

42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4374

43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4474

(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4674

IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4774

47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

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53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 41: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4174

41

Defnton of 1eamp n Pamptc Moent Ccte

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4274

42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4374

43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4474

(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4674

IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4774

47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

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65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

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67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 42: Plate Girder

7182019 Plate Girder

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42

87 Degn Strength n Benng 3Fampe(re4

he atored design moment M at any setion in a eamdue to

external ations shall satisy

876 Laterally Supported Beam

he design ending strength as go$erned y plasti

strength M d shall e taen as

M d = β b Z p f y γ m0 le 12 Z e f y γ m0

876 Holes in the tension zone

( Anf Agf ) ge (f y f u) (γ m1 γ m0 ) 9 54

7182019 Plate Girder

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43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4474

(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4674

IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4774

47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

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51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

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52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

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6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 43: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4374

43

Lterampamp+ St$ampt+ of Be

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4474

(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4674

IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4774

47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

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72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 44: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4474

(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG

44

PamptcRnge IneamptcRnge

Eamptc Rnge

Mp

My

Mcr

Un$rce Length L

Mo Mo

L

Be B(c)ampng Beh-or

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4674

IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4774

47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

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GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

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Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 45: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4574

LATERAL (FLIG gt3 (EA

45

bullF$Camp amp B( Camp+((+bull+istance between lateral supports to thecompression angebullestraints at the ends and at intermediatesupport locations -boundary conditions)bull

ype and position of the loadsbulloment gradient along the unsupported lengthbullype of crosssectionbullonprismatic nature of the memberbullaterial properties

bullagnitude and distribution of residual stressesbullnitial imperfections of geometry andeccentricity of loading

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4674

IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4774

47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

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66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 46: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4674

IILARIT (ET6EE gtL (FLIGAD LATERAL (FLIG gt3 (EA

46

Coamp(n Be

Short n Aamp coreon ttnent of (h ampo

Benng n the ampne of ampo n ttnngamptc cct+

Long n Intamp hortenng n ampteramp $(c)ampng

Intamp -ertcamp efampectonn ampteramp toronamp$(c)ampng

P(re fampe(ramp oe F(ncton of ampenerne

Co(ampe ampterampefampecton n ttf(ncton of ampenerne

Both h-e tenenc+ to famp $+ $(c)ampng n ther e)er ampne

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4774

47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 47: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4774

47

Beam buckling

EI x gtEI y

EI x gtGJ

SIMILARIT1 OF COLUMN BUCKLING AND BEAM BUCKLING 6

M θ

u

M

Section -

u P

P

Section -

$

Column buckling

ampl

y (

l

)gt

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 48: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4874

LATERAL TgtRIgtAL (FLIG gt3ETRI ETIgt

48

$ssumptions for the ideal -basic) case

Beam undistorted

(lastic beha0iour

Loading by e1ual and opposite moments in theplane of the web

o residual stresses(nds are simply supported 0ertically and laterally

he bending moment at which a beam fails by

lateral buckling when sub2ected to uniformend

moment is called its elastic critical moment-cr)

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 49: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 4974

49

34 ORIGINAL BEAM 3$4 LATERALL1 BUCKLED BEAM

M

Plan

Elevationl

M

Section

(a)

θ

Lateal election

y

(b)

$iampting

x

Section

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 50: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5074

3ATgtR A33ETIG LATERAL TA(ILIT

50

upport Conditions

e3ecti0e -unsupported) length

Le0el of load application

stabili4ing or destabili4ing 5

ype of loading

niform or moment gradient 5

hape of crosssectionopen or closed section 5

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 51: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5174

51

877 Lterampamp+ Un(orte Be

The egn $enng trength of ampterampamp+ (n(orte $e

g-en $+

M d = b Z p f bd

f bd = egn tre n $enng o$tne f bd = χLT f y γ m0

χLT 2 re(cton fctor to cco(nt for ampteramp toronamp

$(c)ampng g-en $+

LT = lt76 for roampampe ecton

LT 2 lt for eampe ecton

Cont

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 52: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5274

52

8776 Eamptc Lteramp Toronamp B(c)ampng Moent

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 53: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5374

53

(FF(C6( L$($L ($

Pro0ision of proper lateral bracing impro0es lateral

stability+iscrete and continuous bracing

Cross sectional distortion in the hogging moment region

+iscrete bracing

Le0el of attachment to the beam

Le0el of application of the trans0erse load

ype of connection

Properties of the beams

Bracing should be of su7cient sti3ness to producebuckling between braces

u7cient strength to withstand force transformed bybeam before connecting

gtther 3ailure odes

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 54: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5474

gtther 3ailure odes

54

Sher +eampng ner (ort

9e$ $(c)ampng 9e$ crampng

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 55: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5574

6eb (uc)lig

55

01

d 2

d 2 b3 n3

Effective width for web bucklin

c f t )3n3b( b P +=

t

d 0

t

ampd 4 1

yr

ampt

t 3ampt

y

yr

yr

d 4 1

yr

asymp=

===

==λ

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 56: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5674

6eb rilig

56

bH lt

Hlt$ sloe

Root radius

Sti beaing lengt

y f t )n3b( crip P +=

ELEET gt3 PLATE GIRDER

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 57: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5774

ELEET gt3 PLATE GIRDER

57

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 58: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5874

GEERAL gtIDERATIgt

58

DESIGN OF STRUCTURAL STEEL MEMBERS IS MOSTL

A MATTER OF ROIDING STABILIT BOT LOCALL

IN OERALL SENSE

MOST OF OT TOLLED SECTIONS ARE SO

ROORTIONED TAT LOCAL STABILIT IS NOT ACONSIDERATION

ROBLEM ARISE IN LATE GIRDER BECAUSE OF DEE

TIN WEBS

ONE WA OF IMORING TE LOAD CARRING

CAACIT OF SLENDER LATE IS TO ROIDE

STIFFNERS

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 59: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 5974

gtDE gt3 3AILRE gt3 PLATE GIRDER

59

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 60: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6074

gtDE gt3 3AILRE gt3 PLATE GIRDER

60

IELDING OF TENSION FLANGE BUCKLING OF COMRESSION FLANGE

BUCKLING OF WEB DUE TO SEAR

BUCKLING OF WEB UNDER COMRESSION DUE TO

CONCENTRATED LOAD SEAR IELD OF WEB

BUCKLING OF FLANGE

COMRESSION BUCKLING CAN TAKE LACE IN ARIOUS

WAS

1 ERTICAL BUCKLING INTO WEB

2 FLANGE LOCAL BUCKLING

3 LATERAL TORSIONAL BUCKLING

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 61: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6174

61

MODES

OF

FAILURE

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 62: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6274

Tesio 3ield Actio

62

The resultig shear stresses o aelemet oamp a web are equivalet toricial stresses oe Tesile ad

oe omressive at J to theshear stress$

T i 3i ld A ti

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 63: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6374

Tesio 3ield Actio

63

gtce a web ael has buc)led ishear it loses its resistace to carryadditioal comressive stresses$

gt the other had tesile ricialstress cotiues to icrease i straii the diagoal directio$

Such a panel has a considerable post buckling strength

since increase in tension is limited only by yield stress

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 64: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6474

64

(amp F(L+ $Camp

I this ostbuc)lig rage a ew loadcarryig mechaism is develoed wherebyay additioal shear load is carried by aiclied tesile membrae stress 8eld$ This

tesio 8eld achors agaist the to adbottom fages ad agaist the trasversesti0eers o either side oamp the web ael$

The loadcarryig actio oamp the late girdertha becomes similar to that oamp the truss

I the ostbuc)lig rage the resistaceo0ered by the web lates is aalogous tothat oamp the diagoal tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 65: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6574

65

(amp F(L+ $Camp

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 66: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6674

66

(amp F(L+ $Camp

Prior to Buckling Post Buckling Collapse

Phases of behavior up to collapse of a typical panel in shear

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 67: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6774

67

The loadcarryig actio oamp the lategirder tha becomes similar to that oampthe truss

I the ostbuc)lig rage theresistace o0ered by the web latesis aalogous to that oamp the diagoal

tie bars i the truss$

(amp F(L+ $Camp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 68: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6874

T ti0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 69: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 6974

Trasverse ti0eers

69

Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$

I the 8rst lace they icrease thebuc)lig resistace oamp the web7

ecodly they must cotiue to remai

e0ective aampter the web buc)les to rovideachorage ampor the tesio 8eld7

8ally they must revet ay tedecyampor the fages to move towards oe

aother$

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 70: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7074

i0

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 71: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7174

Trasverse ti0eers

71

I 3igure H the sti0eers have remaiedstraight$

I 3igure lt the sti0eer has ampailed ad has

bee uable to limit the buc)lig to thead1acet subaels oamp the girder7 isteadthe buc)le has ru through the sti0eerositio extedig over both aels$

osequetly sigi8cat reductio i theampailure load oamp the girder occurred$

Tlt) )amp) = gt) $ +)=+) amp lt))$amp ))amp=+ $ lt) +amp) $ lt) )gt $

))amp )gt gt=amp

W(B PampPampamp

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 72: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7274

72

W(B PampPampamp

otatios

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 73: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7374

6eb Proortioig

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage

Page 74: Plate Girder

7182019 Plate Girder

httpslidepdfcomreaderfullplate-girder-569222faef233 7474

6eb Proortioig

Deth gtverall girder deth D willusually be i the rage

L5H le D le L5lt 3gtR GIRDER I (ILDIG

L12 le D le L18 FOR GIRDERS IN IGWA BRIDGES

L10 le D le L15 FOR GIRDERS IN RAILWA BRIDGES

3lage Area oamp fage Aamp B 5ampy x d+ x mo

The breadth b will usually be i therage