N.W.F.P. University of Engineering and Technology Peshawar Lecture 06: Tension Members By: Prof Dr.
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N.W.F.P. University of Engineering and Technology Peshawar Lecture 06: Tension Members By: Prof Dr. Akhtar Naeem Khan [email protected] 1 Topics to be Addressed Types of Steel Structures Introductory concepts Design Strength Net Area at Connection Shear Lag Phenomenon ASD and LRFD Design of Tension Members Design Examples CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 2 Types of steel structures The form of a tension member is 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 of steel structures CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 4 Types of steel structures CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 5 Types of steel structures CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 6 Types of steel structures CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 7 Types of steel structures CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 8 Types of steel structures CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 9 Sections for Tension Members CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 10 Sections for Tension Members CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 11 Design Stresses for Base Material CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 12 Introductory Concepts Stress: The stress in an axially loaded tension member is given by Equation The stress in a tension member is uniform throughout the cross-section except: near the point of application of load, and at the cross-section with holes for bolts or other discontinuities, etc. CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 13 Types of steel structures Gusset plate b Section b-b b 7/8 in. diameter hole a a 8 x ½ in. bar CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan Section a-a 14 Types of steel structures Gusset plate b Section b-b b 7/8 in. diameter hole a a 8 x ½ in. bar Section a-a Area of bar at section a – a = 8 x ½ = 4 in2 Area of bar at section b – b = (8 – 2 x 7/8 ) x ½ = 3.12 in2 The unreduced area of the member is called its gross area = Ag The reduced area of the member is called its net area = An CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 15 Design strength • A tension member can fail by reaching one of 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 Design strength 1. Excessive deformation can occur due to the yielding of the gross section at section a-a Gusset plate b b Sectio 7/8 in. diameter hole a a 8 x ½ in. bar CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan Sectio 17 Design strength 2. Fracture of the net section can occur if the stress at the net section (section b-b) reaches the ultimate stress Fu Gusset plate b b Sec 7/8 in. diameter hole a a 8 x ½ in. bar CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan Se 18 Design strength Yielding of the gross section will occur when the stress f reaches Fy P f Fy Ag Nominal yield strength = Pn = Ag Fy • Fracture of the net section will occur after the stress on the net section area reaches the ultimate stress Fu P f Fu Ae Nominal fracture strength = Pn = Ae Fu CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 19 Design strength • AISC/ASD Ft = 0.6 Fy Ft = 0.5 Fu on Gross Area on Effective Area • AISC/LRFD Design strength for yielding on gross area øtPn =øt Fy Ag = 0.9 Fy Ag Design strength for fracture of net section øtPn = øtFu Ae = 0.75 Fu Ae CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 20 Effective Net Area • The connection has a significant influence on the performance of a tension member. • A connection almost always weakens the member and a measure of its influence is called joint efficiency. CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 21 Effective Net Area •Joint efficiency is a function of: (a) Material ductility (b) Fastener spacing (c) Stress concentration at holes (d) Fabrication procedure (e) Shear lag. CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 22 Effective Net Area Research indicates that shear lag can be accounted for by using a reduced or effective net area Ae CG For Bolted Connections x1 U 1 x L x2 • For bolted connection, the effective net area is Ae = U An • For welded connection, the effective net area is Ae = U Ag CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 23 Effective Net Area • For W, M, and S shapes with width-to-depth ratio of at least 2/3 and for Tee shapes cut from them, if the connection is through the flanges with at least three fasteners per line in the direction of applied load , U= 0.9 • For all other shapes with at least three fasteners per line , U= 0.85 • For all members with only two fasteners per line U= 0.75 CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 24 Net Area Example Example : A 5 x ½ bar of A572 Gr. 50 steel is used as a tension member. It is connected to a gusset plate with six 7/8 in. diameter bolts as shown in below. Assume that the effective net area Ae equals the actual net area An and compute the tensile design strength of the member. Gusset plate b b 7/8 in. diameter bolt a a 5 x ½ in. bar A572 Gr. 50 CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 25 Net Area Example Gross section area (Ag): Ag = 5 x ½ = 2.5 in2 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 calculating net area = 15/16 + 1/16 in. = 1 in. Net section area = An = (5 – 2 x (1)) x ½ = 1.5 in2 CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 26 Net Area Example Gross yielding design strength: ft Pn = ft Fy Ag = 0.9 x 50 ksi x 2.5 in2 = 112.5 kips Fracture design strength: ft Pn = ft Fu Ae = 0.75 x 65 ksi x 1.5 in2 = 73.125 kips Assume Ae = An (only for this problem) Therefore, design strength = 73.125 kips (net section fracture controls). CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 27 Shear Lag in Tension Members • Shear lag in tension members arises when all the elements of a cross section do not participate in the load transfer at a connection. •There are two primary phenomena that arise in these cases: (i) Non-uniform straining of the web resulting in biaxial stress states (ii) Effective area reduction. CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 28 Shear Lag in Tension Members CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 29 Shear Lag in Tension Members Effective area reduction CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 30 Shear Lag in Tension Members Design 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 the connection and the arrangement of crosssection elements that do not participate directly in the connection load transfer. CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 31 Block 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 Block Shear in Tension Members A failure in which the member fails in tension on one section and in shear on the perpendicular section. CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 33 Block Shear in Tension Members (a) T (b) T Shear failure (c) Tension failure CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 34 Block Shear in Tension Members CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 35 Block Shear in Tension Members For such a failure to occur, there are two possible mechanisms: (1) Shear rupture + tensile yielding; and (2) Shear yielding + tensile rupturing. CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 36 Block Shear in Tension Members AISC/ASD Ft = 0.6 Fy on Gross Area Ft = 0.5 Fu on Effective Area Connecting element allowable stresses where failure may be by shear Fv = 0.3 Fu Allowable block shear F = 0.3 Fu + 0.5 Fu CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 37 Block Shear in Tension Members AISC/LRFD øtRn = 0.75(0.6 Fy Agv + Fu Ant) øtRn = 0.75(0.6 Fu Anv + Fy Agt) CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 38 Block Shear in Tension Members Design Bottom Line As a likely limit state for connections, block shear must be considered in design. This can be accomplished by considering the strength limit states of the two failure mechanisms outlined above. CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 39 Design Example 1-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 40 Design Example 1-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 41 Design Example 1-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 42 Design Example 1-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 43 Design Example 1-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 44 Design Example 1-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 45 Design Example 1-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 46 Design Example 1-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 47 Design Example 1-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 48 Design Example 1-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 49 Design Example 1-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 50 Design Example 1-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 51 Design Example 1-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 52 Design Example 1-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 53 Design Example 1-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 54 Design Example 1-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 55 Design Example 2-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 56 Design Example 2-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 57 Design Example 2-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 58 Design Example 2-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 59 Design Example 2-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 60 Design Example 2-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 61 Design Example 2-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 62 Design Example 2-ASD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 63 Design Example 2-ASD Design Alternative 2 CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 64 Design Example 2-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 65 Design Example 2-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 66 Design Example 2-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 67 Design Example 2-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 68 Design Example 2-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 69 Design Example 2-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 70 Design Example 2-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 71 Design Example 2-LRFD CE-409: Lecture 06 Prof. Dr Akhtar Naeem Khan 72