PROBLEM 7.1 For the given state of stress, determine the normal and shearing stresses exerted on the oblique face of the shaded triangular element shown. Use a method of analysis based on the equilibrium of that element, as was done in the derivations of Sec. 7.2. SOLUTION Stresses Areas Forces F = 0: σ A − 15 A sin 30° cos 30° − 15A cos 30° sin 30° + 10A cos 30 cos 30° = 0 σ = 30 sin 30° cos 30° − 10 cos 2 30° σ = 5.49 ksi ΣF = 0: τ A + 15 A sin 30° sin 30° − 15 A cos 30° cos 30° − 10 A cos 30° sin 30° = 0 τ = 15(cos 2 30° − sin 2 30°) + 10 cos 30° sin 30° τ = 11.83 ksi PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced, or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. A student using this manual is using it without permission. PROBLEM 7.4 For the given state of stress, determine the normal and shearing stresses exerted on the oblique face of the shaded triangular element shown. Use a method of analysis based on the equilibrium of that element, as was done in the derivations of Sec. 7.2. SOLUTION Stresses Areas Forces ΣF = 0: σ A + 18 A cos 15° sin 15° + 45 A cos 15° cos 15° − 27 A sin 15° sin 15° + 18A sin 15° cos 15° = 0 σ = −18 cos 15° sin 15° − 45 cos 2 15° + 27sin 2 15° − 18 sin 15° cos 15° σ = −49.2 MPa ΣF = 0: τ A + 18 A cos 15° cos 15° − 45 A cos 15° sin 15° − 27 A sin 15° cos 15° − 18 A sin 15° sin 15° = 0 τ = −18(cos 2 15° − sin 2 15°) + (45 + 27) cos 15° sin 15° τ = 2.41 MPa PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced, or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. A student using this manual is using it without permission. PROBLEM 7.5 For the given state of stress, determine (a) the principal planes, (b) the principal stresses. SOLUTION σ x = −60 MPa σ y = −40 MPa τ xy = 35 MPa (a) tan 2θ p = 2τ xy σx −σ y = (2) (35) = −3.50 −60 + 40 2θ p = −74.05° (b) σ max, min = = σx +σy 2 θ p = −37.0°, 53.0° ± −60 − 40 ± 2 σx −σ y 2 2 −60 + 40 2 2 + τ xy 2 + (35) 2 = −50 ± 36.4 MPa σ max = −13.60 MPa σ min = −86.4 MPa PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced, or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. A student using this manual is using it without permission. PROBLEM 7.8 For the given state of stress, determine (a) the principal planes, (b) the principal stresses. SOLUTION σ x = −8 ksi σ y = 12 ksi τ xy = 5 ksi (a) tan 2θ p = 2τ xy σx − σy 2(5) = −0.5 −8 − 12 = 2θ p = −26.5651° (b) σ max, min = = σx + σy 2 ± −8 + 12 ± 2 = 2 ± 11.1803 θ p = −13.3°, 76.7° 2 σx − σy 2 +τ xy 2 −8 − 12 2 2 + (5)2 σ max = 13.18 ksi σ min = −9.18 ksi PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced, or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. A student using this manual is using it without permission. PROBLEM 7.19 A steel pipe of 12-in. outer diameter is fabricated from 14 -in. -thick plate by welding along a helix that forms an angle of 22.5° with a plane perpendicular to the axis of the pipe. Knowing that a 40-kip axial force P and an 80-kip ⋅ in. torque T, each directed as shown, are applied to the pipe, determine σ and τ in directions, respectively, normal and tangential to the weld. SOLUTION 1 d 2 = 6 in., t = 0.25 in. 2 c1 = c2 − t = 5.75 in. d 2 = 12 in., c2 = ( π J = (c 2 ) π − c ) = (6 2 A = π c22 − c12 = π (62 − 5.752 ) = 9.2284 in 2 4 2 4 1 4 − 5.754 ) = 318.67 in 4 Stresses: σ =− P A 40 = −4.3344 ksi 9.2284 Tc τ= 2 J (80)(6) = = 1.5063 ksi 318.67 σ x = 0, σ y = −4.3344 ksi, τ xy = 1.5063 ksi =− Choose the x′ and y ′ axes, respectively, tangential and normal to the weld. Then σ w = σ y′ and τ w = τ x′y′ θ = 22.5° σ y′ = σx +σy σx −σ y cos 2θ − τ xy sin 2θ 2 2 (−4.3344) [ −(−4.3344)] = − cos 45° − 1.5063 sin 45° 2 2 = −4.76 ksi τ x′y′ = − − σ w = −4.76 ksi σx −σy sin 2θ + τ xy cos 2θ 2 [ −(−4.3344)] =− sin 45° + 1.5063 cos 45° 2 = −0.467 ksi τ w = −0.467 ksi PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced, or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. A student using this manual is using it without permission. PROBLEM 7.22 Two steel plates of uniform cross section 10 × 80 mm are welded together as shown. Knowing that centric 100-kN forces are applied to the welded plates and that the in-plane shearing stress parallel to the weld is 30 MPa, determine (a) the angle β, (b) the corresponding normal stress perpendicular to the weld. SOLUTION Area of weld: Aw = = (a) Fs = 0: Fs − 100sin β = 0 τw = Fs Aw sin β cos β = (b) 30 × 106 = (10 × 10−3 )(80 × 10−3 ) cos β 800 × 10−6 2 m cos β Fs = 100sin β kN = 100 × 103 sin β N 100 × 103 sin β = 125 × 106 sin β cos β −6 800 × 10 / cos β 1 30 × 106 sin 2β = = 0.240 2 125 × 106 Fn = 0: Fn − 100cos β = 0 β = 14.34° Fn = 100cos14.34° = 96.88 kN Aw = 800 × 10−6 = 825.74 × 10−6 m 2 cos14.34 σ = Fn 96.88 × 103 = = 117.3 × 106 Pa Aw 825.74 × 10−6 σ = 117.3 MPa PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced, or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. A student using this manual is using it without permission. PROBLEM 7.31 Solve Probs. 7.5 and 7.9, using Mohr’s circle. PROBLEM 7.5 through 7.8 For the given state of stress, determine (a) the principal planes, (b) the principal stresses. PROBLEM 7.9 through 7.12 For the given state of stress, determine (a) the orientation of the planes of maximum in-plane shearing stress, (b) the maximum in-plane shearing stress, (c) the corresponding normal stress. SOLUTION σ x = −60 MPa, σ y = −40 MPa, τ xy = 35 MPa σ ave = σx +σy 2 = −50 MPa Plotted points for Mohr’s circle: X : (σ x , −τ xy ) = ( −60 MPa, − 35 MPa) Y : (σ y , τ xy ) = (−40 MPa, 35 MPa) C : (σ ave , 0) = ( −50 MPa, 0) (a) GX 35 = = 3.500 CG 10 = 74.05° 1 = − β = −37.03° 2 = 180° − β = 105.95° 1 = α = 52.97° 2 tan β = β θb α θa 2 θb = −37.0° θ a = 53.0° 2 R = CG + GX = 102 + 352 = 36.4 MPa (b) (a′) σ min = σ ave − R = −50 − 36.4 σ min = −86.4 MPa σ max = σ ave + R = −50 + 36.4 σ max = −13.6 MPa θ d = θ B + 45° = 7.97° θ d = 8.0° θe = θ A + 45° = 97.97° θe = 98.0° τ max = R = 36.4 MPa (b′) σ ′ = σ ave = −50 MPa τ max = 36.4 MPa σ ′ = −50.0 MPa PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced, or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. A student using this manual is using it without permission. PROBLEM 7.35 Solve Prob. 7.13, using Mohr’s circle. PROBLEM 7.13 through 7.16 For the given state of stress, determine the normal and shearing stresses after the element shown has been rotated through (a) 25° clockwise, (b) 10° counterclockwise. SOLUTION σ x = 0, σ y = 8 ksi, τ xy = 5 ksi σ ave = σx +σy 2 = 4 ksi Plotted points for Mohr’s circle: X : (0, − 5 ksi) Y : (8 ksi, 5 ksi) C : (4 ksi, 0) FX 5 = = 1.25 FC 4 2θ p = 51.34° tan 2θ p = 2 2 R = FC + FX = 42 + 52 = 6.40 ksi (a) θ = 25° . 2θ = 50° ϕ = 51.34° − 50° = 1.34° σ x′ = σ ave − R cos ϕ (b) θ = 10° . σ x′ = −2.40 ksi τ x′y′ = R sin ϕ τ x′y′ = 0.15 ksi σ y′ = σ ave + R cos ϕ σ y′ = 10.40 ksi 2θ = 20° ϕ = 51.34° + 20° = 71.34° σ x′ = σ ave − R cos ϕ σ x′ = 1.95 ksi τ x′y′ = R sin ϕ τ x′y′ = 6.07 ksi σ y′ = σ ave + R cos ϕ σ y′ = 6.05 ksi PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced, or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. A student using this manual is using it without permission. PROBLEM 7.39 Solve Prob. 7.17, using Mohr’s circle. PROBLEM 7.17 The grain of a wooden member forms an angle of 15° with the vertical. For the state of stress shown, determine (a) the in-plane shearing stress parallel to the grain, (b) the normal stress perpendicular to the grain. SOLUTION σ x = −4 MPa σ y = −1.6 MPa τ xy = 0 σ ave = σx + σy 2 = −2.8 MPa Plotted points for Mohr’s circle: X : (σ x , − τ xy ) = (−4 MPa, 0) Y : (σ y , τ xy ) = (−1.6 MPa, 0) C : (σ ave , 0) = (−2.8 MPa, 0) θ = −15°. 2θ = −30° CX = 1.2 MPa R = 1.2 MPa (a) τ x′y′ = −CX ′ sin 30° = − R sin 30° = −1.2sin 30° (b) σ x′ = σ ave − CX ′ cos 30° = −2.8 − 1.2 cos 30° τ x′y′ = −0.600 MPa σ x′ = −3.84 MPa PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced, or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. A student using this manual is using it without permission. PROBLEM 7.44 Solve Prob. 7.22, using Mohr’s circle. PROBLEM 7.22 Two steel plates of uniform cross section 10 × 80 mm are welded together as shown. Knowing that centric 100-kN forces are applied to the welded plates and that the in-plane shearing stress parallel to the weld is 30 MPa, determine (a) the angle β, (b) the corresponding normal stress perpendicular to the weld. SOLUTION σx = P 100 × 103 = = 125 × 106 Pa = 125 MPa A (10 × 10−3 )(80 × 10−3 ) σy = 0 τ xy = 0 From Mohr’s circle: 30 = 0.48 62.5 (a) sin 2β = (b) σ = 62.5 + 62.5cos 2β β = 14.3° σ = 117.3 MPa PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced, or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. A student using this manual is using it without permission. PROBLEM 7.98 A spherical gas container made of steel has a 5-m outer diameter and a wall thickness of 6 mm. Knowing that the internal pressure is 350 kPa, determine the maximum normal stress and the maximum shearing stress in the container. SOLUTION d = 5 m t = 6 mm = 0.006 m, r = σ = d − t = 2.494 m 2 pr (350 × 103 Pa)(2.494 m) = = 72.742 × 106 Pa 2t 2(0.006 m) σ = 72.7 MPa σ max = 72.742 MPa σ min ≈ 0 (Neglecting small radialstress) τ max = 1 (σ max − σ min ) 2 τ max = 36.4 MPa PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced, or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. A student using this manual is using it without permission. PROBLEM 7.109 The unpressurized cylindrical storage tank shown has a 163 -in. wall thickness and is made of steel having a 60-ksi ultimate strength in tension. Determine the maximum height h to which it can be filled with water if a factor of safety of 4.0 is desired. (Specific weight of water = 62.4 lb/ft 3.) SOLUTION d 0 = (25)(12) = 300 in. 1 3 d − t = 150 − = 149.81 in. 2 16 σ 60 ksi σ all = U = = 15 ksi = 15 × 103 psi F .S . 4.0 pr σ all = t 3 3 tσ all ( 16 ) (15 × 10 ) p= = = 18.77 psi = 2703 lb/ft 2 r 149.81 r= But p = γ h, h= p γ = 2703 lb/ft 2 62.4 lb/ft 3 h = 43.3 ft PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced, or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. A student using this manual is using it without permission.
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