Chapter4 Allowable Stresse
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Transcript of Chapter4 Allowable Stresse
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4-Chapter
Allowable stresses
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contents
Introduction 2.6.1(p8) Compression element, Axial or
bending
Axial tension Allowable shear stress qall Axial compression
Bending stress
Allowable crippling stress in web qall
Combined stresses Back(home)
http://localhost/var/www/apps/conversion/tmp/scratch_3/chapter1-Introdution.ppthttp://localhost/var/www/apps/conversion/tmp/scratch_3/chapter1-Introdution.ppt -
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Introduction
The actual stresses in any part of steel
bridge must not exceed the elastic limit of
the material otherwise permanentdeformation would occur. All structural
calculations are approximate even if all
loads are carefully considered. In trussesneglect the secondary stresses due to the
rigidity of joints.
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The forces in members are determined under the
assumption that the connections are hinge and the
forces along the members are axial. Only the primarystresses can be calculated. In some cases the
secondary stresses may reach 3060 % of the
primary stresses. The analyses neglect also the
torsion in the main girders due to the deflections ofthe X-girders. The unequal distribution of stresses
over the cross section due to bolts holes hasnt taken
into consideration
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The allowable stresses (maximum stresses used in the
calculation) must therefore be lower than the elastic limit.
The more accurate calculations of steel bridge and the
better shop work, the higher allowable stresses may betaken. Also, in the calculation if all possible forces are
taken into account the allowable stresses can be taken
higher than in case that only D.L., L.L, and Impact are
considered.
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The permissible stresses for standard grade
structural steel determined according to the grade of
steel. Structural sections shall be classified,depending on dw/tw for web and c/tf for flanges
under compression, axial bending, to compact,
noncompact, and slender sections as shown Fig(4-1)
Figure-4.1
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Fy and Fu (t/cm2) depend on the thickness
t(1.4-p2).
Grade of
steel
t40mm 100mm t >400mm
Fy
Fu
Fy
Fu
ST37
2.40
3.60
2.15
3.40
ST44
2.80
4.40
2.55
4.10
ST52
3.60
5.20
3.35
4.90
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2.2.1(p6) Primary + additional stresses (wind load
or earthquake loads, lateral shock, etc.)
2.2.3(p7) Additional stresses
Additional stresses (allowable) = Primary
stress 1.20
2.3(p7) Secondary stresses in truss members
1. Chord member's depth > 1/10 of their length.
Diagonal member's depth > 1/15 of their length.
2. Truss with sub-panel.
Reduce 20 % of the allowable stress
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2.6.1(p8) Compression element, Axial or
bending
yF
Factorand
Selender
NoncompactCompact
f
f
w
w
t
C
t
d
Factor depends on:
1. Support of element ((One side (unstiffened
element) or two sides (stiffened element))
and shape of the cross section, I, C, , L, etc.
2. Load on element [(N) or (M) or (M+N)]
(p9,10,11-Table 2.1.a,b&c)
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2.6.2(p13) Axial tension
yyy
y FFFmmtmm
FmmtF get,1.4clauserom10040
4058.0Ft
Hence for,
25ST/10.2F
44ST/60.1F37ST/40.1F
40
2
t
2
t
2
t
cmt
cmtcmt
mmt
25ST/00.2F
44ST/50.1F37ST/30.1F
10040
2
t
2
t
2
t
cmt
cmtcmt
mmtmm
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2.6.3(p13) Allowable shear stress
qall
yall Fget1.4,clauserom1004040
35.0q FFmmtmm
FmmtF
y
y
y
Hence for,
25ST/26.1q
44ST/98.0q
37ST/84.0q
40
2all
2all
2all
cmt
cmt
cmt
mmt
25ST/17.1q
44ST/89.0q
37ST/75.0q
10040
2
all
2all
2all
cmt
cmt
cmt
mmtmm
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2.6.3.1(p13) Effective web area
Rolled section = Total height twBuilt up section = Web height tw2.6.3.2(p14) Shear buckling of web
yw
w
F
105
t
d
dd1
Stiffened web
2q34.54K1
2q
434.5K1
d1
d
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Unstiffened web = Kq = 5.34
If 80.0,F
K45
t
dq
y
q
w
w
no web buckling occur qp = 0.35 Fy
If, F
K
45t
d
y
q
w
w
Check web buckling
yqbq
yqbq
ybq
q
yw
w
q
F35.0
90.0
q20.1
F35.0625.050.1q20.180.0
F35.0q80.0
K
F
57
td
(no web buckling occur)
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2.6.4(p15) Axial compression
r
lk
1.4F40
40
10
)75.058.0(58.0F y
2
4cfromget
mmt
mmtFF
yy
2c 000065.040.1F 2c 000055.030.1F
2c 000085.060.1F 2c 000075.050.1F
2c 000135.01.2F 2c 000125.00.2F
Gradeof steel
Fc (t/cm2)
ST37
ST44
ST52
t 40 mm 40 < t < 100 mm
Fc (t/cm2)
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- For compact and Non-compact
sections use full area(Table2.1-p9-11).
- For slender sections use effectivearea(Tables 2.3&2.4-p23&24).
- For one angle reduce Fc
by 40
%(p15).
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2.6.5(p16) Bending stress
1- For compact sections and the laterally
unsupported length (Lu )of the compression flange islimited by:
(Lu is the smaller of)
- Box sections
Or
fy
u bF
L 84
y
fu
F
b
M
ML
2
184137
I-shape sections
y
fu
F
bL
20 b
y
f
u CFd
bL 1380
Or
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Cb From Table2.2
- Then
Fb = 0.64 Fy (Mx ) Boxand I-shapes Clause 2.6.5.1
Fb = 0.72 Fy (My) I-shapes Clause 2.6.5.2
Fb = 0.64 Fy (My) Box shapes Clause 2.6.5.3
1- 1- For Non-compact sections:
Fb = 0.58 Fy (Mx & My) Box shapes Clause 2.6.5.4
2- 2- For slender (Box and I-shapes) and Non-compact (I-
shapes) sections:
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Tension Clause 2.6.5.5
Fbt = 0.58 Fy
- Compression Clause 2.6.5.5
1- Lu Lall
Fbc = 0.58 Fy
2- Lu > Lall
i( Shallow thick flanged section Luxtf/ bfxd >10 (P18))
For any value of
(eq 2.23)
ii - ( Deep thin flanged section Luxtf/ bfxd
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t
u
y
b
r
L
F
C84
(eq2.24)yltb FF 58.02
y
b
t
u
y
b
F
C
r
L
F
C18884
(eq 2.25)yyb
yTultb FFC
FrLF 58.0
10176.1
)/(64.0 5
2
2
y
b
t
u
F
C
r
L188
(eq2.26)ybTu
ltb FCrL
F 58.0)/(
1200022
(eq2.27)yltbltbltb FFFF 58.02
221
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- II - For Channels( p21) Fltb;
(eq2.29)
)(58.0/
800xyb
fultb MFC
AdLF
III - For slender sections use effective width (be)
and the stress for non-compact(p21).
- Effective width be for slender sections(Table
2.3& 2.4p23&24);
1
2
f
f
)2.3(11112.0116
5.022 TableK
For any value of get from tables 2.3, and 2.4 for
stiffened and unstiffened elements respectively.
K
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Calculate K
Ftb y
44
/ (plate slenderness)
0.105.015.0 2 Calculate
bbe =
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bfu
ltb CAdL
F
/
8001
t
u
y
b
r
L
F
C84 yltb FF 58.02
y
b
t
u
y
b
F
C
r
L
F
C18884
y
b
yTultb F
C
FrLF
5
2
210176.1
)/(64.0
y
b
t
uFC
rL 188 b
Tu
ltb CrL
F 22 )/(
12000
22
21 ltbltbltb FFF yltb FF 58.0
Summary Table for Lateral Torsional Buckling
(Lu > Lall)
For all
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2.6.6 (p22)Allowable crippling stress in web qall
yycrp Fget1.4,clauseromFmm40t
mm40tF75.0F
In tension members we get smaller cross
sections by using high tensile stresses St. 52.
While in compression members we get smallersection if l/i is less than 100 but if l/i is more than
100 we get same section for all kinds of steel.
2.6.7 Combined stressesIn a continuous beam we have a state of
combined shear and bendingback
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pcpt ffqff
F
22,1
22
This stress may be greater than the bending stress
in the outside fibers.
The modern theory of equivalent structure is givenby;
pte fqfF 10.13 22
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2.6.7.1- Axial Compression And Bending
0.121 bcy
bcy
bcx
bcx
c
ca
F
f
F
f
F
f
1.015.0 21 c
ca
F
fWhen
EY
ca
my
EX
ca
mx
F
f
C
F
f
C
1
,
1
21
2EY2
7500F,
7500
EXF
Cmx , Cmy from code
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2.6.7.2- Axial Tension And Bending
0.1bty
bty
btx
btx
t
ta
Ff
Ff
Ff