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A comprehensive set of solved problems and exercises related to the mechanics of materials subject. It covers various topics, including stress and strain, axial loading, torsion, and composite shafts. Detailed solutions and explanations for each problem, making it a valuable resource for students studying this subject. It is particularly useful for preparing for exams or understanding complex concepts.
Typology: Exams
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Date: 2021/04/28 Time: 08:10-09:
200 mm
100 mm 400 mm 200 mm 400 mm
Figure (1)
Solution: Geometry
The lever arm rotates through an angle of ๐ = ( 1805 ยฐ) ฯ rad = 0.8727 rad. Since ฮธ is small, the displacements of points A, C, and D can be approximated by
๐ฟ๐ด = 100 ร ( 1805 ยฐ) ฯ = 8.7266 mm
๐ฟ๐ถ = 400 ร ( 1805 ยฐ) ฯ = 34.9066 mm
๐ฟ๐ท = 600 ร ( 1805 ยฐ) ฯ = 52.3599 mm Average Normal Strain The unstretched length of wires AH, CG, and DF are LAH = 200 mm , LCG = 400 mm , and LDF = 400 mm. We obtain (๐๐๐ฃ๐)๐ด๐ป = (^) ๐ฟ๐ฟ๐ด๐ป๐ด = 8.7267 200 = ๐. ๐๐๐๐ mm/mm Ans.
(๐๐๐ฃ๐)๐ถ๐บ = (^) ๐ฟ๐ฟ๐ถ๐บ๐ถ = 34.9066 400 = ๐. ๐๐๐๐ mm/mm Ans.
(๐๐๐ฃ๐)๐ท๐น = (^) ๐ฟ๐ฟ๐ท๐น๐ท = 52.3599 400 = ๐. ๐๐๐๐ mm/mm Ans.
15 m
Figure (2)
Solution: Internal Loading By considering the equilibrium of the pile with reference to its entire free-body diagram. We have +โ โ ๐น๐ฆ = 0; ๐น + 1882 ร 15 โ 1750 = 0 โน ๐น = ๐๐๐ kN Ans. Also, ๐(๐ฆ) = 18815 ๐ฆ = 12.53๐ฆ kN/m The normal force developed in the pile as a function of y can be determined by considering the equilibrium of the sectional of the pile with reference to its free-body diagram. +โ โ ๐น๐ฆ = 0; 340 + 12 (12.53๐ฆ)๐ฆ โ ๐(๐ฆ) = 0 โน ๐(๐ฆ) = 6.267๐ฆ^2 + 340 kN Displacement The cross-sectional area of the pile is ๐ด = ฯ 4 ร 0.3^2 = 0.0225ฯ m2. We have ฮด = โซ 0 L A(y)EP(y) dy= โซ 0 15 (6.267y0.0225ฯ(29.0)(10^2 +340)(10 (^93) )) dy= โซ 0 15 [3.057(10โ6)๐ฆ^2 + 165.863(10โ6)]๐๐ฆ
= [1.019(10โ6)๐ฆ^3 + 165.863(10โ6)๐ฆ] 015 = ๐. ๐๐๐ mm Ans.
L + ฮด
uB C
Elements ( 1 )
Elements ( 2 )
Figure (4)
Solution (a) Stresses ฯ 1 and ฯ 2 Equilibrium โ ๐น๐ฅ = 0; ๐น 2 = ๐น 1 (1) Element force - deformation behavior: ๐ 1 = (^) 2๐ด๐ธ๐ฟ ๐ 2 = (^) 3๐ด๐ธ2๐ฟ
Geometry of deformation: ๐ 1 + ๐ 2 = โ๐ฟ (3) Combine (1), (2) and (3) ๐ฟ๐น 2๐ด๐ธ +^
2๐ฟ๐น 3๐ด๐ธ = โ๐ฟ โ ๐น = โ^
6๐ด๐ธ 7๐ฟ ๐ฟ Stresses
โ6๐ด๐ธ7๐ฟ ๐ฟ
๐๐ฌ ๐๐ณ ๐น^ Ans.
โ6๐ด๐ธ7๐ฟ ๐ฟ 3 2 ๐ด^
(b) Displacement uB
Figure (5)
Solution d 1 = 35 mm = 0.035 m ; d2 = 50 mm = 0.05 m ; Gb = 36 GPa ; Gs = 80 GPa ; ฯb = 31 MPa ; ฯs = 52 MPa ; (a) ๐ผ๐๐ = 32 ๐ ๐ 14 = 1.4732 ร 10โ7^ ๐^4 ; ๐ผ๐๐ = 32 ๐ (๐ 24 โ ๐ 14 ) = 4.6627 ร 10โ7^ ๐^4 ๐๐ = ๐ ( (^) ๐บ๐๐ผ๐บ๐๐๐+๐บ๐ผ๐๐๐ ๐ผ๐๐ ) and ๐๐ = ๐ ( (^) ๐บ๐๐ผ๐๐๐บ๐ ๐ผ+๐บ๐๐ ๐ ๐ผ๐๐ ) (1)
๐๐โ๐๐๐ฅ = 2๐๐ ๐๐ผ 1 ๐๐ ; ๐๐ โ๐๐๐ฅ = 2๐ ๐๐ ๐ผ 2 ๐๐ (2) (2) into (1), and solving for Tmax for either brass or steel Tmax,b = 2 ฯb d 1 Ipb (GbIpb Gb+IpbGsIps ) = 2096. 44 Nโm
Tmax,s = 2 ฯ dsI 2 ps (GbIpb Gs+IpsGsIps ) = 1107. 73 Nโm โ(controls)
so Tmax = 1107.73 Nโm Ans. (b) LetT = 1150 Nโm , so Tmax = T Expand Ips and Ipb in above expression for T max,s, then for required diameter d 2 T = 2ฯs[^ 32 ฯ(d^24 โd^14 )] d 2 {
Gb( 32 ฯd 14 )+Gs[ 32 ฯ(d 24 โd 14 )] Gs[ 32 ฯ(d 24 โd 14 )] } โ ๐ 2 = 0.05052 ๐ = 50.52 ๐๐ Take an integer and must be greater than 50.52 mm , so ๐ ๐ = ๐๐ ๐๐ Ans.