Plate Girder
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Transcript of Plate Girder
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PLATE GIRDER
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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$4t le 7=
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oditio ampor (eam Lateral tability
37
Laterally upported Beam The desig bedig stregth oamp beams
adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered
by the yield stress
Laterally nsupported Beams
6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted
beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth
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L+)+ =$) 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
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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
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
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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
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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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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(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
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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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2
A girder is a fexural member which isrequired to carry heavy loads orelatively log sas
7182019 Plate Girder
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3
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7182019 Plate Girder
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7182019 Plate Girder
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7182019 Plate Girder
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7182019 Plate Girder
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7182019 Plate Girder
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10
7182019 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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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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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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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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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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(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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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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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 $e on MoentRotton Chrctertc
LAI3IATIgt
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LAI3IATIgtgt3 Rgt
ETIgt
32
C$-)$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
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
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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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(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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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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7182019 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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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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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
7182019 Plate Girder
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5
7182019 Plate Girder
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6
7182019 Plate Girder
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7182019 Plate Girder
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9
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10
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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
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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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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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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
7182019 Plate Girder
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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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(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
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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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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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7182019 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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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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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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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 $+
LT = lt76 for roampampe ecton
LT 2 lt for eampe ecton
Cont
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8776 Eamptc Lteramp Toronamp B(c)ampng Moent
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(FF(C6( L$($L ($
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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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
7182019 Plate Girder
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7
7182019 Plate Girder
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8
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9
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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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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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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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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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(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
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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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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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8
7182019 Plate Girder
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9
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10
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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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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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(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+ $Camp
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T ti0
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Trasverse ti0eers
69
Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$
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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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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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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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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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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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
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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Defnton of 1eamp n Pamptc Moent Ccte
7182019 Plate Girder
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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
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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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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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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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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8776 Eamptc Lteramp Toronamp B(c)ampng Moent
7182019 Plate Girder
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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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(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
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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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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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10
7182019 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$
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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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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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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 $V d
Md B Mdv
M dv= design bending strength under high
shear as defined in section 9
876 Degn Benng Strength (ner 0gh Sher
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Defnton of 1eamp n Pamptc Moent Ccte
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87 Degn Strength n Benng 3Fampe(re4
he atored design moment M at any setion in a eamdue to
external ations shall satisy
876 Laterally Supported Beam
he design ending strength as go$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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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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(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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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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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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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 $e on MoentRotton Chrctertc
LAI3IATIgt
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LAI3IATIgtgt3 Rgt
ETIgt
32
C$-)$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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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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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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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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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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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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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) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp
)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $
lt) )-$+ )$amp
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T+e of Eampeent T+e ofSecton Camp of Secton
Pamptc 3 64Coct
3 74Secoct 3 84
O(ttn eampeent of
coreon fampnge
Roampampe $t le $t le 6lt= $t le 6=gt
9eampe $t le 8 $t le $t le 6
Internamp eampeent of
coreon fampnge
$enng $t le 7 $t le = $t le 7
Aamp co not ampc$ampe $t le 7
9e$ NA t
etht le 8lt t le 6lt= t le 67
Angampe $enng
Aamp
co
Crc(ampr t($e th
o(ter eter D
Dt le 7 Dt le 7 Dt le 88 7
T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent
y f
250=ε
$tle
$tle
6lt=
$tle
6=gt
not ampc$ampe $t le 6=gt
3$4t le 7=
7182019 Plate Girder
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oditio ampor (eam Lateral tability
37
Laterally upported Beam The desig bedig stregth oamp beams
adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered
by the yield stress
Laterally nsupported Beams
6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted
beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth
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38
L+)+ =$) gt)+
L+)+ =amp=$) gt)+
LUSAS L+)+ T$$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 $V d
Md B Mdv
M dv= design bending strength under high
shear as defined in section 9
876 Degn Benng Strength (ner 0gh Sher
7182019 Plate Girder
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41
Defnton of 1eamp n Pamptc Moent Ccte
7182019 Plate Girder
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42
87 Degn Strength n Benng 3Fampe(re4
he atored design moment M at any setion in a eamdue to
external ations shall satisy
876 Laterally Supported Beam
he design ending strength as go$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$ampt+ of Be
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(ECA4IgtR gt3 E(ER (ETED Tgt (EDIG
44
PamptcRnge IneamptcRnge
Eamptc Rnge
Mp
My
Mcr
Un$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)
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
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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$e Length o ompression Flanges
8amp Shear
8 Stiened e +anels
81 nd +anels design
82 nd +anels designed using ension ield ation
8 -nhor ores
8 Design o Beams and +late Girders ith Solid es
81 0inimum e hiness
82 Setional +roperties
8 Flanges Cont
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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING
8 Stiener Design
81 General
82 Design o 3ntermediate rans$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) $$$amp
$ lt) $-)$amp + +amp $+ )$amp +amp
+lt)) lt) = $+ +amp ++ lt )-
$+ +amp )amp) )$amp + gt) =gt) $ $ $+
gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)
+=+) $+ +amp ++ = gt) )=) $ +$
lt) $gt $ $+ gt=amp
+) )))amp $ + $-)$amp + gt=) $+ =) $ $))
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33
+) )))amp $ + $ )$amp + gt=) $+ =) $ $))
)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt
amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp
=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+
3711 Wlt)amp + +amp+ =) lt) )gt) lt+
gt) ++gt) $ $amp + ltamp) lt =)amp
$+$amp ++ (= lt$= $+ gt=amp $
)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)
gt)$) $+$amp $ lt) +=) )lt+amp
3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+
gt) ++gt) $ ))$amp lt) ) ) =amp)
$)$amp lt$= $+ gt=amp
372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp
+) )amp) + $$
a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)
7182019 Plate Girder
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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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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
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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
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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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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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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
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
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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
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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$e Length o ompression Flanges
8amp Shear
8 Stiened e +anels
81 nd +anels design
82 nd +anels designed using ension ield ation
8 -nhor ores
8 Design o Beams and +late Girders ith Solid es
81 0inimum e hiness
82 Setional +roperties
8 Flanges Cont
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SECTION 8 DESIGN OF MEMBERS SUBJECTED TO BENDING
8 Stiener Design
81 General
82 Design o 3ntermediate rans$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) $$$amp
$ lt) $-)$amp + +amp $+ )$amp +amp
+lt)) lt) = $+ +amp ++ lt )-
$+ +amp )amp) )$amp + gt) =gt) $ $ $+
gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)
+=+) $+ +amp ++ = gt) )=) $ +$
lt) $gt $ $+ gt=amp
+) )))amp $ + $-)$amp + gt=) $+ =) $ $))
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33
+) )))amp $ + $ )$amp + gt=) $+ =) $ $))
)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt
amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp
=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+
3711 Wlt)amp + +amp+ =) lt) )gt) lt+
gt) ++gt) $ $amp + ltamp) lt =)amp
$+$amp ++ (= lt$= $+ gt=amp $
)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)
gt)$) $+$amp $ lt) +=) )lt+amp
3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+
gt) ++gt) $ ))$amp lt) ) ) =amp)
$)$amp lt$= $+ gt=amp
372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp
+) )amp) + $$
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
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)
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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
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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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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) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp
)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $
lt) )-$+ )$amp
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T+e of Eampeent T+e ofSecton Camp of Secton
Pamptc 3 64Coct
3 74Secoct 3 84
O(ttn eampeent of
coreon fampnge
Roampampe $t le $t le 6lt= $t le 6=gt
9eampe $t le 8 $t le $t le 6
Internamp eampeent of
coreon fampnge
$enng $t le 7 $t le = $t le 7
Aamp co not ampc$ampe $t le 7
9e$ NA t
etht le 8lt t le 6lt= t le 67
Angampe $enng
Aamp
co
Crc(ampr t($e th
o(ter eter D
Dt le 7 Dt le 7 Dt le 88 7
T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent
y f
250=ε
$tle
$tle
6lt=
$tle
6=gt
not ampc$ampe $t le 6=gt
3$4t le 7=
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oditio ampor (eam Lateral tability
37
Laterally upported Beam The desig bedig stregth oamp beams
adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered
by the yield stress
Laterally nsupported Beams
6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted
beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth
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38
L+)+ =$) gt)+
L+)+ =amp=$) gt)+
LUSAS L+)+ T$$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
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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
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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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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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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
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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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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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(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 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
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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 $V d
Md B Mdv
M dv= design bending strength under high
shear as defined in section 9
876 Degn Benng Strength (ner 0gh Sher
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41
Defnton of 1eamp n Pamptc Moent Ccte
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87 Degn Strength n Benng 3Fampe(re4
he atored design moment M at any setion in a eamdue to
external ations shall satisy
876 Laterally Supported Beam
he design ending strength as go$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
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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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(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
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19
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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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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$4t le 7=
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oditio ampor (eam Lateral tability
37
Laterally upported Beam The desig bedig stregth oamp beams
adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered
by the yield stress
Laterally nsupported Beams
6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted
beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth
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L+)+ =$) 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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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
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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) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp
)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $
lt) )-$+ )$amp
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T+e of Eampeent T+e ofSecton Camp of Secton
Pamptc 3 64Coct
3 74Secoct 3 84
O(ttn eampeent of
coreon fampnge
Roampampe $t le $t le 6lt= $t le 6=gt
9eampe $t le 8 $t le $t le 6
Internamp eampeent of
coreon fampnge
$enng $t le 7 $t le = $t le 7
Aamp co not ampc$ampe $t le 7
9e$ NA t
etht le 8lt t le 6lt= t le 67
Angampe $enng
Aamp
co
Crc(ampr t($e th
o(ter eter D
Dt le 7 Dt le 7 Dt le 88 7
T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent
y f
250=ε
$tle
$tle
6lt=
$tle
6=gt
not ampc$ampe $t le 6=gt
3$4t le 7=
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oditio ampor (eam Lateral tability
37
Laterally upported Beam The desig bedig stregth oamp beams
adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered
by the yield stress
Laterally nsupported Beams
6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted
beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth
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L+)+ =$) gt)+
L+)+ =amp=$) gt)+
LUSAS L+)+ T$$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 $+
LT = lt76 for roampampe ecton
LT 2 lt for eampe ecton
Cont
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52
8776 Eamptc Lteramp Toronamp B(c)ampng Moent
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53
(FF(C6( L$($L ($
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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(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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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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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) $$$amp
$ lt) $-)$amp + +amp $+ )$amp +amp
+lt)) lt) = $+ +amp ++ lt )-
$+ +amp )amp) )$amp + gt) =gt) $ $ $+
gt=amp S=lt $-)$amp +) amp$ $ltgt) gt= lt)
+=+) $+ +amp ++ = gt) )=) $ +$
lt) $gt $ $+ gt=amp
+) )))amp $ + $-)$amp + gt=) $+ =) $ $))
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+) )))amp $ + $ )$amp + gt=) $+ =) $ $))
)) Tlt) $+ gt=amp +amp gt) +$) gt)$) lt) +) +lt)) gt
amp lt) lt $ ltamp) +$ $ )+lt )))amp $ + $-)$amp
=gt)) $ $)$amp =) $ ++ $) $)amp $ lt)+
3711 Wlt)amp + +amp+ =) lt) )gt) lt+
gt) ++gt) $ $amp + ltamp) lt =)amp
$+$amp ++ (= lt$= $+ gt=amp $
)amp+gt) lt) )gt=$amp $ gt)ampamp $)amp )=)
gt)$) $+$amp $ lt) +=) )lt+amp
3712 Wlt)amp )+ +amp+ =) lt) )gt) lt+
gt) ++gt) $ ))$amp lt) ) ) =amp)
$)$amp lt$= $+ gt=amp
372 Oamp gt+ $ lt) +gt$) $= +) $ )$amp
+) )amp) + $$
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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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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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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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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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) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp
)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $
lt) )-$+ )$amp
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T+e of Eampeent T+e ofSecton Camp of Secton
Pamptc 3 64Coct
3 74Secoct 3 84
O(ttn eampeent of
coreon fampnge
Roampampe $t le $t le 6lt= $t le 6=gt
9eampe $t le 8 $t le $t le 6
Internamp eampeent of
coreon fampnge
$enng $t le 7 $t le = $t le 7
Aamp co not ampc$ampe $t le 7
9e$ NA t
etht le 8lt t le 6lt= t le 67
Angampe $enng
Aamp
co
Crc(ampr t($e th
o(ter eter D
Dt le 7 Dt le 7 Dt le 88 7
T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent
y f
250=ε
$tle
$tle
6lt=
$tle
6=gt
not ampc$ampe $t le 6=gt
3$4t le 7=
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oditio ampor (eam Lateral tability
37
Laterally upported Beam The desig bedig stregth oamp beams
adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered
by the yield stress
Laterally nsupported Beams
6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted
beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth
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38
L+)+ =$) gt)+
L+)+ =amp=$) gt)+
LUSAS L+)+ T$$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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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 $+
LT = lt76 for roampampe ecton
LT 2 lt for eampe ecton
Cont
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52
8776 Eamptc Lteramp Toronamp B(c)ampng Moent
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(FF(C6( L$($L ($
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
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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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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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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
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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
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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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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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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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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) + $$
a) Class 1 (Plastic) mdash C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)
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34
a) Class 1 (Plastic) C$-)$amp ltlt +amp ))$ + ltamp) +amp lt+)
lt) $+$amp ++ )=) $ +=) $ lt) ==) gt $+$amp $ +
)lt+amp Tlt) lt $ ltamp) +$ $ +) )))amp lt+ gt) ) lt+amp
lt+ )) =amp) C+ 1 (+ amp T+gt) 2 $ IS 800
b) Class 2 (C$+ C$-)$amp ltlt +amp ))$ + $)amp $
)+amp) gt= lt+) amp+)=+) + ltamp) $+$amp ++ $ $+$amp $
+ )lt+amp =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +)
)))amp lt+ gt) ) lt+amp lt+ )) =amp) C+ 2 (C$+ gt= )+)
lt+amp lt+ )) =amp) C+ 1 (+ amp T+gt) 2
c) Class 3 (Semi-compact) mdash C$-)$amp amp ltlt lt) ))) gt) amp
$)$amp +amp )+lt ) ) gt= +ampamp$ ))$ lt) + $)amp $
)+amp) =) $ $+ gt=amp Tlt) lt $ ltamp) +$ $ +) )))amp
lt+ gt) ) lt+amp lt+ )) =amp) C+ 3 (S)-$+ gt= )+) lt+amp
lt+ )) =amp) C+ 2 (C$+ amp T+gt) 2
d) Class 4 (Slender) mdash C$-)$amp amp ltlt lt) )))amp gt=) $+ ))amp
gt)$) )+ltamp ) ) Tlt) lt $ ltamp) +$ $ +) )))amp
lt+ gt) )+) lt+amp lt+ )) =amp) C+ 3 (S)-$+ amp T+gt) 2
Iamp =lt +) lt) ))) )$amp $ )amp lt+ gt) +=+) )lt) gt
$$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
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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
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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
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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$4t le 7=
7182019 Plate Girder
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oditio ampor (eam Lateral tability
37
Laterally upported Beam The desig bedig stregth oamp beams
adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered
by the yield stress
Laterally nsupported Beams
6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted
beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth
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38
L+)+ =$) 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
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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
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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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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 $V d
Md B Mdv
M dv= design bending strength under high
shear as defined in section 9
876 Degn Benng Strength (ner 0gh Sher
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Defnton of 1eamp n Pamptc Moent Ccte
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42
87 Degn Strength n Benng 3Fampe(re4
he atored design moment M at any setion in a eamdue to
external ations shall satisy
876 Laterally Supported Beam
he design ending strength as go$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
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
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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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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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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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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)
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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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
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
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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
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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
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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
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
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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) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp
)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $
lt) )-$+ )$amp
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T+e of Eampeent T+e ofSecton Camp of Secton
Pamptc 3 64Coct
3 74Secoct 3 84
O(ttn eampeent of
coreon fampnge
Roampampe $t le $t le 6lt= $t le 6=gt
9eampe $t le 8 $t le $t le 6
Internamp eampeent of
coreon fampnge
$enng $t le 7 $t le = $t le 7
Aamp co not ampc$ampe $t le 7
9e$ NA t
etht le 8lt t le 6lt= t le 67
Angampe $enng
Aamp
co
Crc(ampr t($e th
o(ter eter D
Dt le 7 Dt le 7 Dt le 88 7
T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent
y f
250=ε
$tle
$tle
6lt=
$tle
6=gt
not ampc$ampe $t le 6=gt
3$4t le 7=
7182019 Plate Girder
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oditio ampor (eam Lateral tability
37
Laterally upported Beam The desig bedig stregth oamp beams
adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered
by the yield stress
Laterally nsupported Beams
6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted
beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth
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38
L+)+ =$) gt)+
L+)+ =amp=$) gt)+
LUSAS L+)+ T$$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
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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
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
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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$
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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
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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$4t le 7=
7182019 Plate Girder
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oditio ampor (eam Lateral tability
37
Laterally upported Beam The desig bedig stregth oamp beams
adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered
by the yield stress
Laterally nsupported Beams
6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted
beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth
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38
L+)+ =$) 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
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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
7182019 Plate Girder
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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
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
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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) $$amp $ IS 801 $ +$=amp $ lt) $-$+-gt=amp
)amplt $ gt )=amp lt $ lt) $)$amp +) )))amp amp )) $
lt) )-$+ )$amp
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T+e of Eampeent T+e ofSecton Camp of Secton
Pamptc 3 64Coct
3 74Secoct 3 84
O(ttn eampeent of
coreon fampnge
Roampampe $t le $t le 6lt= $t le 6=gt
9eampe $t le 8 $t le $t le 6
Internamp eampeent of
coreon fampnge
$enng $t le 7 $t le = $t le 7
Aamp co not ampc$ampe $t le 7
9e$ NA t
etht le 8lt t le 6lt= t le 67
Angampe $enng
Aamp
co
Crc(ampr t($e th
o(ter eter D
Dt le 7 Dt le 7 Dt le 88 7
T$ampe 7 Lt on 9th to Thc)ne Rto of Pampte Eampeent
y f
250=ε
$tle
$tle
6lt=
$tle
6=gt
not ampc$ampe $t le 6=gt
3$4t le 7=
7182019 Plate Girder
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oditio ampor (eam Lateral tability
37
Laterally upported Beam The desig bedig stregth oamp beams
adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered
by the yield stress
Laterally nsupported Beams
6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted
beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth
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38
L+)+ =$) gt)+
L+)+ =amp=$) gt)+
LUSAS L+)+ T$$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
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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
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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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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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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
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
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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
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
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
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
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
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+ $Camp
7182019 Plate Girder
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T ti0
7182019 Plate Girder
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Trasverse ti0eers
69
Trasverse sti0eers lay a imortatrole i allowig the ampull ultimate loadresistace oamp a late girder to beachieved$
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
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
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
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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$
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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
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
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
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
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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)
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
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$
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
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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
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
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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
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
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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
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
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
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$4t le 7=
7182019 Plate Girder
httpslidepdfcomreaderfullplate-girder-569222faef233 3774
oditio ampor (eam Lateral tability
37
Laterally upported Beam The desig bedig stregth oamp beams
adequately suorted agaist lateral torsioalbuc)lig laterally suorted beam+ is govered
by the yield stress
Laterally nsupported Beams
6he a beam is ot adequately suortedagaist lateral buc)lig laterally usuorted
beams+ the desig bedig stregth may begovered by lateral torsioal buc)lig stregth
7182019 Plate Girder
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38
L+)+ =$) 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
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
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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
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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
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
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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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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