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    N.W.F.P. University of Engineering and

    Technology Peshawar

    Lect ure 06: Tens ion Members

    1

    By: Prof Dr. Akhtar Naeem Khan

    [email protected]

    Types of Steel Structures

    Introductory concepts

    Top ic s t o be Addressed

    Design Strength

    Net Area at Connection

    Shear Lag Phenomenon

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 2

    ASD and LRFD Design of TensionMembers

    Design Examples

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    The form of a tension member is

    Types o f s t ee l s t ruc t ures

    governed to a large extent by

    Type of structure of which it is a part

    Method of joining it to connecting portions.

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 3

    Types o f s t ee l s t ruc t ures

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 4

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    Types o f s t ee l s t ruc t ures

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 5

    Types o f s t ee l s t ruc t ures

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 6

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    Types o f s t ee l s t ruc t ures

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 7

    Types o f s t ee l s t ruc t ures

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 8

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    Types o f s t ee l s t ruc t ures

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 9

    Sec t ions for Tension Members

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 10

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    Sec t ions for Tension Members

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 11

    Design St resses

    for

    Base Mat er ia l

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 12

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    In t roduc t o ry Concep ts

    Stress: The stress in an axially loaded tensionmember is given by Equation

    The stress in a tension member is uniformthroughout the cross-section except:

    near the point of application of load, and

    at the cross-section with holes for bolts or other

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 13

    , .

    Types o f s t ee l s t ruc t ures

    b b

    Gusset plate

    7/8 in . diameter hole

    Section b-bb b

    Gusset plate

    7/8 in . diameter hole

    b b

    Gusset plate

    7/8 in . diameter hole

    Section b-bSection b-b

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 14

    aa

    8 x in. barSection a-a

    aa

    8 x in. bar

    aa

    8 x in. barSection a-aSection a-a

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    Types o f s t ee l s t ruc t ures

    b b

    Gusset plate

    Section b-bb b

    Gusset plate

    b b

    Gusset plate

    Section b-bSection b-b

    2

    aa

    8 x in. bar

    7/8 in. diameter hole

    Section a-a

    aa

    8 x in. bar

    7/8 in. diameter hole

    aa

    8 x in. bar

    7/8 in. diameter hole

    Section a-aSection a-a

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 15

    Area of bar at section b b = (8 2 x 7/8 ) x = 3.12 in2

    The unreduced area of the member is called its gross area = AgThe reduced area of the member is called its net area = An

    Design st rengt h

    A tension member can fail by reaching oneof two limit states:

    1. Excessive deformation Yielding at the gross area

    2. Fracture Fracture at the net area

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 16

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    Design st rengt h

    1. Excessive deformation can occur due to theyielding of the gross section at section a-a

    b b

    7/8 in.

    b b

    7/8 in.

    b b

    7/8 in.

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 17

    aa

    8 x

    aa

    8 x

    aa

    8 x

    Design st rengt h2. Fracture of the net section can occur if the stress

    at the net section (section b-b) reaches theultimate stress Fu

    b b

    7/8 in.

    b b

    7/8 in.

    b b

    7/8 in.

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 18

    aa

    8 x

    aa

    8 x

    aa

    8 x

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    Design st rengt h

    Yielding of the gross section will occur whenthe stress f reaches Fy

    Nominal yield strength = Pn = Ag Fy

    Fracture of the net section will occur after the stress

    y

    g

    FA

    ==f

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 19

    u

    Nominal fracture strength = Pn = Ae Fu

    u

    e

    FAP ==f

    Design st rengt h

    AISC/ASDFt = 0.6 Fy on Gross Area

    Ft = 0.5 Fu on Effective Area

    AISC/LRFD

    Design strength for yielding on gross area

    P = F A = 0.9 F A

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 20

    Design strength for fracture of net section

    tPn = tFu Ae = 0.75 Fu Ae

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    Ef fec t ive Net Area

    The connection has a significant influence on theperformance of a tension member. A connection almost always weakens the memberand a measure of its influence is called jointefficiency.

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 21

    Ef fec t ive Net Area

    Joint efficiency is a function of:

    (a) Material ductility

    (b) Fastener spacing

    (c) Stress concentration at holes

    (d) Fabrication procedure

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 22

    (e) Shear lag.

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    Ef fec t ive Net AreaResearch indicates that shear lag can be accounted for by

    using a reduced or effective net area Ae

    CG

    2x

    1x

    L

    xU = 1

    For Bolted Connections

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 23

    For bolted connection, t e effective net area is Ae = UAn

    For welded connection, the effective net area is Ae = UAg

    Ef fec t ive Net Area

    For W, M, and S shapes with width-to-depth ratio of at least2/3 and for Tee shapes cut from them, if the connection is

    the direction of applied load ,

    U= 0.9

    For all other shapes with at least three fasteners per line ,U= 0.85

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 24

    For all members with only two fasteners per line

    U= 0.75

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    Net Area Ex ampleExample : A 5 x bar of A572 Gr. 50 steel is used as a tension

    member. It is connected to a gusset plate with six 7/8 in. diameterbolts as shown in below. Assume that the effective net area Ae equals

    the actual net area A and com ute the tensile desi n stren th of thenmember.

    b b

    Gusset plate

    7/8 in. diameter bolt

    b b

    Gusset plate

    7/8 in. diameter bolt

    b b

    Gusset plate

    7/8 in. diameter bolt

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 25

    aa

    5 x in. bar

    A572 Gr. 50

    aa

    5 x in. bar

    aa

    5 x in. bar

    A572 Gr. 50

    Net Area Ex ample

    Gross section area (Ag):

    A = 5 x = 2.5 in2g

    Net section area (An):

    Bolt diameter = db = 7/8 in.

    Nominal hole diameter = dh

    = 7/8 + 1/16 in. = 15/16 in.

    Hole diameter for calculatin net area = 15/16 + 1/16 in. = 1 in.

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 26

    Net section area = An

    = (5 2 x (1)) x = 1.5 in2

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    Net Area Ex ample

    Gross yielding design strength:

    t n=

    t yAg

    = 0.9 x 50 ksi x 2.5 in2 = 112.5 kips

    Fracture design strength:

    ftPn = ft Fu Ae= 0.75 x 65 ksi x 1.5 in2 = 73.125 kips

    Assume Ae

    = An

    (only for this problem)

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 27

    Therefore, design strength = 73.125 kips (net section fracture

    controls).

    Shear Lag i n Tension

    Members Shear lag in tension members arises when all theelements of a cross section do not artici ate in theload transfer at a connection.There are two primary phenomena that arise inthese cases:

    (i) Non-uniform straining of the web resulting in

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 28

    ax a s ress s a es(ii) Effective area reduction.

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    Shear Lag i n Tension

    Members

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 29

    Shear Lag i n Tension

    MembersEffective area reduction

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 30

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    Shear Lag i n Tension

    MembersDesign Bottom Line

    Shear lag can have a large influence on the

    strength of tension members , in essence

    reducing the effective area of the section. The

    amount of the reduction is related to the length of

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 31

    -

    section elements that do not participate directly in

    the connection load transfer.

    Bloc k Shear in Tension

    Members

    Block shear is a combined tensile/shear tearing

    out of an entire section of a connection.

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 32

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    Bloc k Shear in Tension

    Members,

    two possible mechanisms:

    (1) Shear rupture + tensile yielding; and

    (2) Shear yielding + tensile rupturing.

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 33

    Bloc k Shear in Tension

    Members

    As a likely limit state for connections,block shear must be considered indesign. This can be accomplished byconsiderin the stren th limit states of

    CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 34

    the two failure mechanisms outlinedabove.

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    Design Ex am ple 1-ASD

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    Design Ex am ple 1-ASD

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    Design Ex am ple 1-ASD

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    Design Ex am ple 1-ASD

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    Design Ex am ple 1-ASD

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    Design Ex am ple 1-ASD

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    Design Ex am ple 1-ASD

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    Design Ex am ple 1-ASD

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    Desig n Ex am ple 1-LRFD

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    Desig n Ex am ple 1-LRFD

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    Desig n Ex am ple 1-LRFD

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    Desig n Ex am ple 1-LRFD

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    Desig n Ex am ple 1-LRFD

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    Desig n Ex am ple 1-LRFD

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    Desig n Ex am ple 1-LRFD

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    Desig n Ex am ple 1-LRFD

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    Design Ex am ple 2-ASD

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    Design Ex am ple 2-ASD

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    Design Ex am ple 2-ASD

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    Design Ex am ple 2-ASD

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    Design Ex am ple 2-ASD

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    Design Ex am ple 2-ASD

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    Design Ex am ple 2-ASD

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    Design Ex am ple 2-ASD

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    Design Ex am ple 2-ASD

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    Design Alternative 2

    Desig n Ex am ple 2-LRFD

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    Desig n Ex am ple 2-LRFD

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    Desig n Ex am ple 2-LRFD

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    Desig n Ex am ple 2-LRFD

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    Desig n Ex am ple 2-LRFD

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    Desig n Ex am ple 2-LRFD

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