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

    back

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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

    back

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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)

    back

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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).

    back

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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

    back

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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