Design of Beam Column [Compatibility Mode]
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Transcript of Design of Beam Column [Compatibility Mode]
Design of Beam gColumn
By
Ass. Prof. Dr. Ehab B. Matar
B C lBeam-Column Nearly all-structural members in building frames or industrial
portal frames are subjected to both bending moments and axial load either in tension or compression formsaxial load either in tension or compression forms
(a) (b) (c)
BEHAVIOR OF BEAM-COLUMN UNDER AXIALBEHAVIOR OF BEAM COLUMN UNDER AXIAL LOAD AND BENDING MOMENT
Behavior of beam column = behavior of beam (considering effect of lateral torsional buckling)
+behavior of columns (considering effect of global
M buckling)M ult
M
M'
M' ult M varies
P = const.
MyM
P
Fig. Relationship for I beam
Modes of failure of Beam- ColumnJohnson [3] has mentioned a number of modes of failure that
characterizes a beam-column behavior which are summarized as follows:follows:
Failure by yielding: in the case of member subjected to bending moment and axial tension force.F il b i t bilit i th l f b di ith t Failure by instability in the plane of bending without twisting for the case of beam-column that is transversely loaded but is stable w.r.t. Lateral torsional buckling.F il b l t l t i l b kli Failure by lateral torsional buckling for beam-column loaded about their strong axis without adequate bracing.
Failure by instability about one of the principle y y p paxes for members subjected to axial compressive force and biaxial bending moment with stiff sections (W-shapes).
Failure by combined twisting and bending for the Failure by combined twisting and bending for the case of thin walled open sections (that are torsionally weak sections) subjected to axial compression force and biaxial bending moment.bending moment.
Design Criteria of Beam-Column
Assessment of Buckling length Effect of P- Effect of P- Design of sections subjected to M,T and
th bj t d t M Nothers subjected to M,N Checking local bucklingg g Preliminary section design
Assessment of Buckling Length
1. Kinds of buckling in beam column: Buckling out of plan (L ): will be Buckling out of plan (Lby): will be
governed by the vertical bracing profileB kli i l (L ) ill b d b Buckling in plan (Lbx): will be governed by the end conditions of the columns and the relative stiffness between different members.
41:10Ex.:- Buckling out of plan
2.5mI 0 23I
1.5m 1 0.7I0.7I
4mI 0.23I
24mVertical wind bracing
Lby=4m
Buckling in PlaneF ll d fi d d di i h b kli l h ld b For well defined end conditions, the buckling length could be estimated as per the following table
Buckling Shape
0.65k values = 0.80 1.00 1.20 2.00 2.10
R i fi d & l i fRotation free & translation fixedRotation fixed & translation fixed
End condition
Rotation free & translation freeRotation fixed & translation free
For Portal Frames: the alignment chart is used to determine the buckling coefficient factor k based on the following assumptions:-assumptions:
All behavior is elastic. The members are prismatic. All columns reach their respective buckling loads
simultaneously. For braced frames (no side sway), the girders are assumed to be For braced frames (no side sway), the girders are assumed to be
in single curvature while for un-braced frames (side sway is permitted), the girders are assumed to be in double curvature.
At a joint the restraining moment provided by the girders is At a joint, the restraining moment provided by the girders is distributed among the columns in proportion to their stiffness.
The girders are elastically restrained at their ends by the l d t th t f b kli th t ti f thcolumns, and at the onset of buckling the rotations of the
girders at its ends are equal and opposite. The girders carry no axial loads.g y
Determine the factor G expressing the relative stiffness at the two ends of the columns as follows:
g
gg
c
cc
LIE
LIE
G
Where EcIc, EgIg are flexural stiffness of the column and girder meeting at a joint while Lc, Lg are the
l d i d l th
g
column and girder lengths It is to be noted based on ECP recommendations
that:that: When the col. End is hinged G=10 When the col End is fixed G=1 0 When the col. End is fixed G=1.0
Alignment Chart
Steps to use alignment chartC l l t th G ffi i t t b th d f th l1. Calculate the G coefficient at both ends of the columns
2. It is to be noted that when the far end of the girder is fixed or hinged a modification factor is to be applied as follows:
The far end is hinged, then multiply EgIg /Lg ratio by 0.5 for the case of side sway is permitted and 1.5 for the case of side sway is preventedis prevented.
The far end is fixed, then multiply EgIg /Lg ratio by 0.67 for case of side sway is permitted and 2.0 for case of side sway is
t dprevented.
3. Decide whether the frame is permitted or prevented from side ec de e e e a e s pe ed o p e e ed o s desway and then use proper alignment chart
upper col. is permitted to sidesway
upper col. is permitted to sidesway
lower& upper col. are lower col. is lower col. is both permitted to sidesway
prevented from sidesway
prevented from sidesway
For truss frame: two options may be adopted1. Treating the column of the frame truss as a column partially
fixed at truss end or2. Solving the truss frame as a portal frame with girder stiffness
50 to 100 times column stiffness50 to 100 times column stiffness.
2a
h
L
50 - 100 Ich'
h'=h+a
Fig.(6.5) Buckling for column-truss framesL
Beam- Column with CraneBeam Column with Crane
ExamplesEx1
Required: Calculate the column b kli l th i l f thbuckling length in plane of the frame if end A is hinged and end D is fixed considering the frameD is fixed considering the frame is permissible to side sway
Solution: B II
1:10
C
For Column AB End A is hinged, then GA=10
B II
7m 1.5 I
C
1.5 I
g , At end B GB = ( ∑Ic/Lc)/( ∑
IG/LG) = (1.5I/7)/(I/26.13) = 5.626m
A D
From the alignment chart with side sway permitted, K = 2.6
Then, Lbx = 2.6x7 = 18.2m
However, on substituting into equation 6.4 for GA and GB K h l f 2 63 t ti f thGB, K approaches a value of 2.63 to satisfy the equality sign.
For Column CD For Column CD End D is fixed, then GD = 1.0
And at end C Gc = ( ∑Ic/Lc)/( ∑ IG/LG) = And at end C Gc = ( ∑Ic/Lc)/( ∑ IG/LG) = (1.5I/7)/(I/26.13) = 5.6
From the alignment chart with side sway permitted K = From the alignment chart with side sway permitted K = 1.72
Then, Lbx = 1.72x7 = 12.04m. Then, Lbx 1.72x7 12.04m. It is worth noting that the fixation at column end has
reduced the buckling length factor K by nearly 33.85% g g y ycompared with hinged case.
Ex2 Given: The shown two story
building frame, knowing that end G and H of the girders is
C I F I H
end G and H of the girders is fixed to the adjacent R.C. shear wall.
Required: Calculate the
3m
B 2 I E 2 I
2 I 2 I
G Shear Wall
Required: Calculate the columns buckling length in plane of the frame if end A is fi d d d D i hi d
7m6m
4m
A
4I
D
3I
fixed and end D is hinged. Solution: For Column AB For Column AB GA = 1.0 (end A is fixed) GB = (4I/4+2I/3)/(2I/6)=5.0 From the alignment chart
for side sway prevented K=0 85K 0.85
Lbx = 0.85 x 4 = 3.4m
For Column DE GD = 10 (end D is hinged) GD = 10 (end D is hinged) GE = (3I/4+2I/3)/(2I/6+2x2I/7) = 1.57 From the alignment chart for side sway
prevented K=0.89prevented K 0.89 Lbx = 0.89 x 4 = 3.56m
Ex.3 Given: The shown truss
frame, knowing that end A is hi d d d B i fi d 3 5mhinged and end B is fixed
Required: Calculate the columns buckling length in plane of the truss frame BA
8m
3.5m
plane of the truss frame. Solution: For Column A
16x2.4=38.4m
9.75m
The buckling length can be found by two different methods:
38 4
9.75m75 Ic
Method 1: assuming the column as hinged – partial fixed to the truss. Then f t bl (5 3) i th
38.4m
from table (5.3) in the Egyptian code K=2.0. The height of the column h’ = 8+3 5/2 = 9 75m8+3.5/2 = 9.75m.
Lbx = 9.75x2.0=19.5m
Method 2: transforming the truss frame into an equivalent gable frame with an assumed large stiffness q g gvalue of the rafter (assumed here 75Ic)
GA = 10 as the column is hinged and GB = (Ic/9.75)/(75Ic/(2x19.3)=0.05 From the alignment chart with side sway permitted
K=1.68 Lbx=1.68x9.75=16.38m The difference in the two methods is referred to the
approximate assumption of modeling the truss stiffness. However in the second method if the truss stiffness isHowever in the second method if the truss stiffness is varied between 50Ic and 100Ic then the K factor will vary between 1.7 and 1.67 respectively.between 1.7 and 1.67 respectively.
For Column B Again the buckling length will be found by two different methods: Method 1: assuming the column as fixed – partial fixed to the
truss. Then from table (5.3) in the Egyptian code K=1.2. Thetruss. Then from table (5.3) in the Egyptian code K 1.2. The height of the column h’ = 8+3.5/2 = 9.75m.
Lbx = 9.75x1.2=11.7mM th d 2 t f i th t f i t i l t bl Method 2: transforming the truss frame into an equivalent gable frame with an assumed large stiffness value of the rafter (assumed here 75Ic)
GA = 1.0 as the column is fixed and GB = (Ic/9.75)/(75Ic/(2x19.3)=0.05 From the alignment chart with side sway permitted K=1 16 From the alignment chart with side sway permitted K=1.16 Lbx=1.16x9.75=11.31m
bPbP
P- EffectcP
b
cPtP tP
f c
b
t
b
f
Sections sub. to M, T Sections sub. To M, NLPLP 23 LPLP 23
EILP
EILP fcb
f 848
3
EILP
EILP ftb
tbf 848
3
AP
ZP
ZLPf cfcb
b
4AP
ZP
ZLPf t
ftb
b 4 AZZ xx
b 4AZZ fxx4
Moment Magnification factor for beamMoment Magnification factor for beam columns prevented from side sway
Assuming that Pe = π2EI/L2 and α = P/Pe y1
W(z)
Py
P
Mo
Lz
Mi
11.1.1 2
0
02
0max LMEIMM z p(y1+ )
L/II
b- Intial B.M.D.
Fig. (6.6) Simplified Analysis of Beam-column
L/2L/II
c- P - effect
1.1 2
0
02
LMEIcm
1m
mcA
mz AMM .0max
Moment Magnification factor for beam gcolumns permitted to side sway
1.. 00max
mm
cMAMM y1
P
IG=infinity
HP
L
1
11 20
2EIcmP
/
L
P( + y1)
4 2
0LMcm H/2
y1
L
H/2
assumed as a qurter sine curveSecondary B.M
4 2PLP
effective length 2L is P
H/2
)2/(
4
3
2
HLLH
EIPL
PP
e
gused in calculating the value of α, Cm
121
2&
3)2/(
32
00
HLEI
HLMEI
LH
164
1 2 HLEILcm
Design of sections subjected to M,T
Failure of these members is governed by yielding
fff y g
N
ptMN
ANf
fff
yxM
netN
MMf
Af
Moreover, the compressive bending stress ynetxnet
M ZZf
shall be checked against the lateral torsional buckling stress.
ExamplesExample 1 Given:-M=20mt, T=15t, St.37, , , ,Beam is restrained laterally at supports Required:- Design of steel beam Required:- Design of steel beam Solution:-
tMN fff
ptx
ptMN
fZM
AT
fff
A;by gmultiplyin then ,
EQptx
x
PAfMZAT ..
x
Assuming A/Zx = 0.07 then: PEQ = 15+20E2x0 07 = 155t PEQ = 15+20E2x0.07 = 155t Areq = PEQ/fpt = 155/1.4 = 110.7cm2
Trying IPE 500 with the following geometrical Trying IPE 500 with the following geometrical properties
Zx = 1930cm3, A = 116cm2, L’ =258.2cm, f 2h=d=50cm, Af=20x1.6=32cm2, rt = 5.17cm
Checking the class of the cross sectionflange is s bjected to p re compression flange is subjected to pure compression
C/tf = (20/2-1.02/2-2.1) /1.6=4.6 O.K. class 1 web is subjected to bending and tension force web is subjected to bending and tension force
therefore < 0.5. Then, a = N/(2tw.Fy)= 3.06cm, , ( y) , , dw/tw = 42.6/1.02 = 41.76
which is smaller than O.K. Class 15.956.63
yFMT y
2/129015 cmtf
ZM
ATff
xMN
2/036.11930
220
/129.0116
cmtEf
cmtf
M
N
the resultant tensile stress is +1.17 t/cm2 < fpt for steel 37, O K
2/91.0&17.1036.1129.0 cmtff MN
O.K. Checking compressive stresses of –0.91 t/cm2, and as the
top flange is braced laterally at supports only which results i t d l th f 500 L 258 2in unsupported length of 500cm > Lumax = 258.2cm therefore, a check for the lateral torsional buckling should be carried out.3 Th ll bl i t i d b th 3- The allowable compressive stress is governed by the lateral torsional buckling stress which is given as the maximum of either:
bfu
ltb CAdL
f ./.
800
ltb
b
cmtxxf
C
/024.10.1.)50(500
328000.1
2
y
b
y
b
t
u
fL
fC
fC
rL
/
84&18871.9617.5
500
2
y
b
ytultb
fcmtxxf
fxCEfrL
f
580/081424.2)71.96(640
.5176.1
./64.0
22
f / 2 f
yltb fcmtxxE
f 58.0/08.14.20.15176.1
64.0
Then fltb = 1.08 t/cm2 and this value < fbc and therefore controls.
Fact=0.91t/cm2<Fbc=1.08t/cm2 => O.k safe
Design of sections subjected to M,N
Failure of these members may be governed by instability bybxca A
fAff
1
my
bcybcxc
cc
Af
Aff
1.. 21
Ey
ca
my
Ex
ca
mx
ffA
ff
cA
1
&1
21
fca = actual compressive stress due to axial compressive force = P/Af h ll bl b kli f h b
EyEx ff
fc = the allowable buckling stress of the member considered as a column
f f = the bending stresses about the x and fbx, fby = the bending stresses about the x and y axes
fbcx, fbcy = the allowable compressive bending stress
Allowable Bending Stresses
The allowable bending stress will depends on:-on:
1. Section ClassL t l t d l th f i2. Lateral un-supported length of compression flange
Local buckling for eccentric Sec.
NThe maximum web to thickness ratio for compact sections are
w
y
w
w
.dthen 0.5for
F/
td
then 0.5 for
663113
699
1- yw F.t
Na2
2- Then determine the value of as follows: yw Ft
The maximum web to thickness ratio for non-compact sections are
y
w
w F/
td
then 1- for
2
190
For rolled section cahdw 2
For welded section Stahd fwyw
wF
)(td
then 1- for
195
For welded section Stad fw 2
Allowable Stresses in Bending
For compact sections bent about major axis64.0 FF ybc bf
138020 ofeither
exccedingnot isLu length dunsupporte lateral max. that thecondition in
Ab
ybcC tf
dw twd
bf
138020
where
CdF
Aor
Fb
by
f
y
f
M1 M2
3.23.005.175.1loadingransversewithout tbeamsfor
*2
11
MM
MMC
tbA
b
fff
For transverse loaded members Cb is taken from table (4.2)For compact section bent about minor axis F =0 72F
g22
MMb
For compact section bent about minor axis Fbc=0.72Fy
concrete slab
composite beam with shear connectorFlange embedded
concrete slab
welded
open web joist
welded or bolted roof purlin
stiffener
bracedunbraced
lateral buckling of floor systemstrut
Types of lateral restraintsTypes of lateral restraints
For Compact sections not satisfying the above limits or Non-Compact sections satisfying the above mentioned limits, Fbc=Fbt=0.58Fy
When the lateral unsupported length Lu exceeds the maximum LuWhen the lateral unsupported length Lu exceeds the maximum Luthen the maximum bending compression Fbc is the min. of either 0.58Fy or max. of either Fltb1 and Fltb2
CF 800
y
btu
bfu
ltb
FCrL
CAdL
F
then84/When
/.1
btu
b
yltb
y
FCrL
FC
F.F
then188/ 84When
5802
wff
fft Atb
btr
6/112/3
yyb
yt
u
ltb
yy
FFCx
FrL
F
FF
58.01017.1
.64.0 5
2
2
y
btu
b
FCrL
Cx
then188/When
1017.1
yb
t
ultb
y
FC
rL
F 58.01200022
continuewhere
7500&750022
yEy
xEx ff
where
factoron modificatimoment
1
m
yx
M
C
loadingansversewithout tr
sway sidefrompreventedframesfor 4.06.02
1
m M
MC
endsat restraint moment and loading transversesway with side from prevented framesfor 85.0
gmC
endsat supportedsimply and loading transversesway with side from prevented framesfor 0.1mC
sway side topermitted framesfor 85.0mC
M2M2
M1
frames prevented from side sway
without transverse loading
frames prevented from side sway
with transverse loading
frames prevented from side sway
with transverse loading
without end moment restraintswith end moment restraintsM1<M2
000022
7500&7500EyEx ff
yx
Preliminary Section DesignBased on the AISC specifications [4] a simplified treatment was carried
out to facilitate the first trial of choosing the beam column cross section.
011 .A.ff
ff
bc
b
c
ca
011
.
ff
cf.ZM
f.AP
E
cam
bcc
bcc
Multiplying the last equation by A.fc
EQcca
m
bc
c Pf.Af
cff
.ZAMP
1
E
cabcf
1
The term (cm/(1-(fca/fE))) may be taken unity & the ratio of A/Z may be
termed B which is given in the steel tables and may roughly be taken equal to
0.07 for most steel sections, then,
bc
cEQ f
f.B.MPP .................................................................(6.23)
h i l b d EQPhil iThus a cross sectional area may be assumed as
c
EQg f
A while a section
modulus can be calculated the same way as before where Z/A14-15
Mff
.AZ.PM
c
bcEQ ..............................................................(6.24)
Thus a trial sectional modulus can be obtained as bc
EQf
MZ
Example 2 Given:- St. 37, shown beam
Case M1 M2 P 1 +20mt +20mt -15t
2 +20mt -20mt -15t
3 +20mt +20mt -60t
4 +80mt +80mt -15t
Required:- Design the beam for different combinations Solution:-
C 2 Case 2 M1= +20mt, M2=-20mt i.e. double curvature, P = -15t
Ass ming that B = A/Z is nearl eq al to 0 07 & Assuming that B = A/Z is nearly equal to 0.07 &the slenderness ratio in the range of 40, and therefore for St.
37 fc will equal to 1.3t/cm2 and while fbc is 1.4t/cm237 fc will equal to 1.3t/cm and while fbc is 1.4t/cm
1453.122007.015.. txExfBMPP cEQ
25.11131
145
4.1
cmf
PA
f
EQreq
bcEQ
If λ = 40, then ix ≥ 500/40 ≥12.5cm
3.1fc
, x
iy ≥ 250/40 i.e. ≥ 6.25 cm, Z > 2000/1 4 i e >1428 6cm3 Zx > 2000/1.4 i.e. >1428.6cm . Try section of I.P.E. 500 may be checked knowing
the following geometrical properties:the following geometrical properties: A = 116 cm2, Zx = 1930 cm3, ix = 20.4cm, iy =
4 31cm r = 5 17cm4.31cm, rt = 5.17cm, Lumax = 258.2cm, h = d = 50cm, Af = 20x1.6 = 32cm2
Checking class of the chosen section; FlangeC/tf = 10/1.6=6.25 yF/.916 = 10.33 O.K class 1
For web; Npw=(50-2x1.6)x1.02x2.4=114.57t >> N=15t. Therefore:
a = N/(2tw.Fy) = 3.06cm,
5707306350 cahd
699an smaller th is which 41.7642.6/1.02dw/tw
57.07.306.322
w cad
O.K. Class 1
4.70)113(
699
yF
2/129015Pf 2
58250&51.24500
/129.011615 cmt
APf
yx
ca
22max /18.1)58(000065.04.1,58
31.44.20
fcmtxfc
yx
2
1
/041220
0.115.0109.0
cmtEMf
Aff
c
ca
/04.11930
cmtZ
fx
bx
As the maximum lateral unsupported length L’=258.2cm for this section,
which is greater than the actual distance between lateral restraints of the
compression flange (250cm), therefore there is no need to check for the lateral
torsional buckling stress Therefore the value of f is controlled by thetorsional buckling stress. Therefore the value of fbc is controlled by the
allowable bending stress, which is 1.4 t/cm2.
0.1. 1 Aff
ff bca
0185004.1129.0
ff bcc
safeO k
0.185.04.118.1
safeO.k
Example 3 12.16mt
5.33
41:10
Given:- 9.5mt
B.M.D
33
0.23I
0.7I0.7I
I
4
21
1:10
1.5m2.5m
4
Vertical wind bracing 24m24m
4m
N.A.
338.7
12 I.P.E. 360
I.P.E. 360
320
360mm
812.7
170
320
the distance between purlins or side girt is restricted to 2m.
Sec. M(mt) N(t)Sec. M(mt) N(t) 1 -16.93(case I) -5.19(case I) 2 0(case I)
-4.72(case II) -11.22(case I) -6.85 (case II)
3 -22.02(case I) -2.66(case I)4 +10.38(case I) -2.13(case I)
Required:-D i th h f i St 52 id i th ff tDesign the shown frame using St. 52 considering the effect of existing knee bracing or not for sections 1 and 3 and compare between the two casescompare between the two cases Solution:-Design of Sec. 1
M = 16.93mt, N = -5.19 t
Considering that λmax will nearly be 80 then fc = 1.24t/cm2.
Calculating the buckling length: Lby = 400cm
For calculating Lbx, the frame is permitted to side sway, GA = 10
(hinged base) and 34122470
8 ../I.
/IG B therefore from the alignment
chart K = 2.5. Thus Lbx = 2.58=20m.
Then for λ = 80, cmi&cmi yx 580
4002580
2000
Hence
75
177512
24129316070195
P
t..
.xE.x..ff
.B.MPP
Q
bc
cEQ
26260
24175 cm..f
PA
c
EQreq
Zx > 16.93E2/2.1 i.e. >806.19cm3.
Case of existing of knee bracing
Knee bracing detail for the rafter
Knee bracing detail for the column
When a knee bracing is used then Lu= the di t b t id i t i 200distance between side girt i.e. 200cm
When there is no knee bracing then Lu= the distance between the point of maximum momentdistance between the point of maximum moment and the point of zero moment i.e. 800cm.
Case 1: no knee bracing Case 1: no knee bracing A trial section of I.P.E.. No. 360 was tried first and
found to be unsafe for low lateral torsional bucklingfound to be unsafe for low lateral torsional bucklingstress, therefore another section of I.P.E. No.500may be checked knowing the following geometrical
tiproperties A = 116cm2, Zx = 1930cm3, ix = 20.4cm, iy =
4 31cm rt = 5 17cm4.31cm, rt = 5.17cm, L’ = 258.2cm, h = d = 50cm, Af = 201.6 = 32cm2
Checking Section class and actual stressesFl C/t 10/1 6 6 25 8 9 O K l 1a- Flange: C/tf=10/1.6=6.25 yF/9.16 =8.9 O.K class 1
b- Web: is subjected to bending moment and compression
force then:force, then:
Npw = (50-21.6) 1.023.6 = 171.85t >> N = 5.19t.
Therefore, a = N/(2tw.Fy)= 0.71cm, 520.cahdw , , ( w y) ,2w ,
dw/tw=42.6/1.02=41.76 which is smaller than 9663113
699 .F)( y
O K Cl 1O.K. Class 1
20450116
195 cm/t..APfca
22 8004980001350120498
8192314
4000498420
2000
cm/t.).(x..f,.
..
&..
cmax
yx
2
1
88029316
01150060
/E.Mf
.A..ff
c
ca
28801930
29316 cm/t.E.ZMf
xbx
As Luact=800cm > Lumax=258cm, a check for lateral torsional buckling is needed as follows
fltb is controlled by the greater value of
21217515080032800800
cm/t...xxC.
d.LA
f bu
fltb
Where: α = 0/16.93 = 0 and Cb = 1.75
or
bltb
y
b
t
u
C.f
fC
..r
L
212000
18874154175
800
b
t
ultb
rL 2
fcm/t.xf 58088075112000 2 yltb f.cm/t.
.f 580880
74154 2
Fbc=1.12 t/cm2.
On checking the stabilit interaction eq ation it as fo nd that the sectionOn checking the stability interaction equation it was found that the section
is safe:
011 .A.ff bca
01840121880
800450
01
....
..
..ff bcc
Case 2: of existing knee bracingSearching for these approximate initial requirements a trial section of
I.P.E. No. 400 may be checked knowing the following geometrical properties: A = 84.5 cm2, Zx = 1160cm3, ix = 16.5cm, iy = 3.95cm, L’ = 189.7cm
Checking class of the chosen section:
a- Flange: C/tf=9/1.35=6.67 yF/.916 =8.9 O.K class 1 b- Web: is subjected to bending moment and compression force, then Npw =
(40-21.35) 0.86 3.6 = 115.48t >> N = 5.19t.
Th f N/(2t F ) 0 84 530hd Therefore, a = N/(2tw.Fy) = 0.84cm, 5302
.cadw ,
dw/tw=33.1/0.86 = 38.49 which is smaller than 5562113
699 .F)(
O.K. 113 F)( y
Class 1
20610584
195 cm/t..
.APfca
22 51021121750021121
27101953
40021121516
2000
/t)/(f
..
&.. yx
1
22
011501190
51021121750021121
.A..ff
cm/t.)./(f,.
c
ca
cmax
24611160
29316 cm/t.E.ZMf
xbx
c
Lumax’=189.7cm < Luact =200cm, therefore there is a need to check for
the lateral torsional buckling stress.
13175030750051751
7509318
697512
2)(C
..
.
13175030750051751 2 .).(x..x..Cb
fltb is controlled by the greater value of
800yb
u
fltb f.cm/t...
x.xxC.
d.LA
f 58075213140200
35118800800 2
Therefore the value of f is controlled by the allowable bending stress forTherefore the value of fbc is controlled by the allowable bending stress for
that type of steel, which is 2.1t/cm2.
O h ki h bili i i i i f d h hOn checking the stability interaction equation it was found that the
section is safe:
4610610
011 .A.ff
ff
bc
b
c
ca
01815012
4615100610 ..
..
..
Therefore on using knee bracing there is a saving on column steel
weights that reach 36.8%.
Design of Sec. 3M = 22.02mt, N = -2.66 t
For the rafter, the effect of the normal force is generally very small and
the rafter may be designed only for bendingthe rafter may be designed only for bending.
Hence:
2123320222 E.MZ 2123312850
cm.x.f
Zbt
req
When knee bracing is used Luact = dist. Between purlins=200cm otherwise
for no knee bracing Luact= distance between the maximum bending moment
and the point of zero moment i.e. 5.33m
Case 1: of no knee bracing
450mmI.P.E. 450 416.19
N.A.
450mm
414 9.4
450
12 I.P.E. 450
416.19
19014.6
Searching for these approximate initial requirements a trial section of built
up section composed of I.P.E. No. 450 + 1/2 I.P.E. No. 450 was tried first and
may be checked knowing the following geometrical properties:
A = 164.084cm2, Zt = 3292.2cm3, Zc = 3059.73cm3, ix = 28.9cm,
iy = 3.91cm, rt = 5.54cm, d = 86.4cm, Af = 19x1.46 = 27.74cm2,
L’ = 200.3cm
cm/t.E.Mfbc272020222
safe K.O.cm/t.cm/t..x.
E.ZMf
cm/t..Z
f
tbt
cbc
22 1279085023292
20222
720733059
.x.Zt 85023292
As Lumax’ = 200.3cm considering that Cb = 1.75 as α = 0 for this section,
< Luact =533cm, therefore there is a need to check for the lateral torsional
buckling stress.
fltb is controlled by the greater value of
28407514865337427800800
cm/t....x
.xC.d.L
Af b
u
fltb
Where: α = 0/22.02 = 0 and Cb =1.75
Or bb CCL 533
ytu
y
b
y
b
t
u
f.r/L
fC
&fC
..r
L
841882196545
533
2
yb
ytultb f.
xCE..f
51761640
f/t.x).(f 58072163632196640 22
yltb f.cm/t..x.xE.
)(.f 580721630151761
640 2
Therefore the lateral torsional buckling fltb = 1.72t/cm2. Therefore the allowable value of fbc is controlled by the lateral torsional buckling stress which is 1.72 t/cm2 which is larger than the actual stress = 0.72 t/cm2 O.K safe.
Case 2 of existing knee bracing
N.A.
360mm 338.7
12 I P E 360
I.P.E. 360
320
170
812.7
2 I.P.E. 360
Searching for these approximate initial requirements a trial section of built
up section composed of I.P.E.. No. 360 + 1/2 I.P.E.. No. 360 was tried and
may be checked knowing the following geometrical properties
A = 118.874cm2, Zt = 2015.73cm3, d = 68cm, 2Af = 17x1.27 = 21.59cm2 , rt = 5.07cm, L’ = 153.35cm
cm/t.E.ZMfbc
28260382000
20222
K.O.cm/t.cm/t..x.
E.ZMf
.Z
tbt
c
22 12291850732015
20222382000
As Lumax’ = 153.35cm considering that Cb = 1.26 as α = -12.16/22.08 =
-0.55 for this section, <Luact=200cm, therefore there is a need to check for the , ,
lateral torsional buckling stress:
fltb is controlled by the greater value of fltb y g
26126168200
5921800800cm/t...
x.xC.
d.LA
f bu
fltb
or
844339075
200fC
.Lu b
212580
075
cm/t.f..f
f.r
yltb
yt
Therefore the value of fbc is controlled by the lateral torsional buckling stress of a value of 2 1 t/cm2 which is greater than the compressive bending stress ofa value of 2.1 t/cm , which is greater than the compressive bending stress of 0.826 t/cm2 . Therefore the chosen section is safe. Although using smaller section may be quite safe but this section satisfies the maximum permissible deflection and any reduction in member stiffness may fall beyond the allowabledeflection and any reduction in member stiffness may fall beyond the allowable deflection limits. However, on using knee bracing there is a saving on rafter steel weights that reach 27.56%
Thank you y&
Good LuckGood Luck
Ass. Prof. Dr. Ehab Boghdadi Matar