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Strength of Materials University of Technology Second Class

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1 Strength of Materials University of Technology Second Class
Building and Construction Engineering Department Strength of Materials Second Class 2014 – 2015 prepared by Professor Dr. Nabeel Al-Bayati Structural Engineering Branch

2 Bending Stresses in Beams
Lecture -7 Bending Stresses in Beams Lecture -7, Part 2 Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

3 Lecture -7-part-2 (Bending Stresses in Beams)
7-11 Bending of Members Made of Several Materials: Consider a composite beam formed from two materials with E1 and E2. Normal strain varies linearly. Piecewise linear normal stress variation. Neutral axis does not pass through section centroid of composite section. Elemental forces on the section are Define a transformed section such that (Ratio of the moduli of elasticity). Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

4 Lecture -7-part-2 (Bending Stresses in Beams)
Solved Example Bar is made from bonded pieces of steel (Es = 29x106 psi) and brass (Eb = 15x106 psi). Determine the maximum stress in the steel and brass when a moment of 40 kip*in is applied. Solution Steps: Step 1: Transform the bar to an equivalent cross section made entirely of brass Step 2: Evaluate the cross sectional properties of the transformed section Step 3: Calculate the maximum stress in the transformed section. This is the correct maximum stress for the brass pieces of the bar. Step 4: Determine the maximum stress in the steel portion of the bar by multiplying the maximum stress for the transformed section by the ratio of the moduli of elasticity. Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

5 Lecture -7-part-2 (Bending Stresses in Beams)
7-12 Reinforced Concrete Beams: Concrete beams subjected to bending moments are reinforced by steel rods. The steel rods carry the entire tensile load below the neutral surface. The upper part of the concrete beam carries the compressive load. In the transformed section, the cross sectional area of the steel, As, is replaced by the equivalent area nAs where n = Es/Ec. To determine the location of the neutral axis, The normal stress in the concrete and steel Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

6 Lecture -7-part-2 (Bending Stresses in Beams)
Solved Example A concrete floor slab is reinforced with 5/8-in-diameter steel rods. The modulus of elasticity is 29x106psi for steel and 3.6x106psi for concrete. With an applied bending moment of 40 kip*in for 1-ft width of the slab, determine the maximum stress in the concrete and steel. Solution Steps: Step 1: Transform to a section made entirely of concrete. Step 2: Evaluate the geometric properties of the transformed section. Step 3: Calculate the maximum stresses. Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

7 Lecture -7-part-2 (Bending Stresses in Beams)
7-13: Solved Examples: Example 7-21:Knowing that a beam of the cross section shown of two materials (Aluminum and steel) is bent about a horizontal axis and that the bending moment is 60 kip.ft, EAL= 10*106 psi and Es = 30*106 psi. determine the maximum stress in each material. Aluminum steel 4in 8in 3in bAL=3in Solution : Transform the section to an equivalent cross section made entirely of steel y’A, in3 y’, in Area, in2 96 40 4 10 8*3 =24 1*4 = 4 1 2 ∑y’A=136 ∑A = 28 steel 4in 8in 1in N.A. y’ 3in Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

8 Lecture -7-part-2 (Bending Stresses in Beams)
Example 7-22:Knowing that a beam of the cross section shown of two materials (Wood and steel) is bent about a horizontal axis and that the (all) wood = 1200psi, (all) steel= 20000psi, EWood= 1.2*106 psi and Es = 30*106 psi. Find the allowable moment. b = 8in 6in 3in 1/2in 12in 3in 6in N.A. 8/25in =0.32in y’ 2 1 3 steel Solution : transform wood section to steel steel 1/2in Wood y’A, in3 y’, in Area, in2 12.75 24.96 0.75 6.5 0.25 2*0.5 =1 12*0.32 =3.84 6*0.5=3 1 2 3 ∑y’A=38.46 ∑A = 7.84 steel Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

9 Lecture -7-part-2 (Bending Stresses in Beams)
N.A. =0.32in y’=4.9 2 1 3 13-4.9 =8.1 13 0.5in =7.6 =4.4 Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

10 Lecture -7-part-2 (Bending Stresses in Beams)
Home Work : Solve the previous example (7-22) by transform steel section to wood Example 7-23: For the beam shown: Draw bending moment diagram along beam Draw stress distribution due to Max Positive Moment only. where EWood= 14kN/mm2 and ESteel = 210 kN/mm2. steel Wood 400mm 200mm 10mm 360mm Section y-y w=10kN/m 4m A B 1.5m hinge M=65kN.m C D y Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

11 Lecture -7-part-2 (Bending Stresses in Beams)
Solution : w=10kN/m Member CD: RC= RD = 10*4/2 = 20 kN MC = 0 , MD = 0, M(mid-span CD) = 10*42/8 = 20kN.m C D RC RD 4m w=10kN/m 40kN.m C A B Member ABC: RA M=65kN.m RC=20kN  MA = , MA *3* *3 = 0, MA = 40kN.m 1.5m 1.5m  MC = , *3 * 1.5 – RA *3 = 0, RA = 50kN x RA=50kN RD=20kN 40kN.m RC=20kN Shear VA = RA = 50kN VB = 50 – 10 *1.5 = 35 VC = 50 – 10 *3 = 20 VD = 50 – 10 * 7 = -20 = RD VA=50kN VD=20kN VC=20kN VB=35kN S.F.D Moment x = 0 to 1.5m MA = - 40kN.m MBA = - 40 – 10*1.5*1.5/2 + 50* 1.5 = 23.75kN.m x = 1.5m to 3m MBC = – 65 = kN.m MC = 0 Mmax (Positive) = kN.m +23.75kN.m +20kN.m A B C D -40kN.m kN.m Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

12 Lecture -7-part-2 (Bending Stresses in Beams)
Wood 6000mm 3000mm 10mm 360mm y’ N.A. 100mm 2 1 3 4 200mm Transform steel sections to wood y’A, mm3 y’, mm Area, mm2 150000 5 =375 360/2+10=190 2/3*360+10=250 3000*10 =30000 6000*10 = 60000 200*360 = 72000 2*(100*360/2)=36000 1 2 3 4 ∑y’A= ∑A = 3000mm Wood 6000mm 10mm 360mm y’=228.94 N.A. 100mm 2 1 3 4 200mm 151.06 Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

13 Lecture -7-part-2 (Bending Stresses in Beams)
400mm A=13.634MPa B=12.73 C=0.848 D=1.317 E=19.76 F=20.66 N.A. Stress distribution at point B due to max. positive moment A 10mm Steel B C c2=151.06 141.06 N.A. Wood 360mm 218.94 c1=228.94 D 10mm Steel E F 200mm Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

14 Lecture -7-part-2 (Bending Stresses in Beams)
Example 7-24: Circular sections of aluminum and steel having maximum bending moment = 80kN.m., where EAluminum= 70*103MPa and ESteel = 21*104 MPa. Find max. bending stress for steel and aluminum and draw stress distribution of the section. Steel Aluminum 150mm 300mm Solution : Transform steel sections to aluminum Steel Aluminum 150mm 300mm 3*150=450mm Steel to Aluminum N.A. 3*150=450mm Steel to Aluminum 150mm Aluminum 300mm R1=150 R2=75 a=75mm b=225mm Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

15 Lecture -7-part-2 (Bending Stresses in Beams)
Steel Aluminum 150mm 300mm A B C D E F N.A. 75mm A=26.827MPa B=13.413 C=40.24 D=40.24 E=13.413 F=26.827 N.A. Stress distribution of the composite section Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)

16 Prof. Dr. Nabeel Al-Bayati
Thank you for listening Prof. Dr. Nabeel Al-Bayati Prof. Dr. Nabeel Al-Bayati Lecture -7-part-2 (Bending Stresses in Beams)


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