Mechanics of Materials

34
C C H H A A P P T T E E R R 7 7

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Mechanics of Materials Solutions

Transcript of Mechanics of Materials

Page 1: Mechanics of Materials

CCHHAAPPTTEERR 77

Page 2: Mechanics of Materials

PROPRIETARY MATERIAL. © 2012 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,

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PROBLEM 7.2

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

0:Σ =F

80 cos55 cos55 40 sin 55 sin 55 0σ − ° ° + ° ° =A A A

2 280 cos 55 40sin 55σ = ° − ° 0.521 MPaσ = −

0:Σ =F

80 cos 55 sin 55 40 sin 55 cos 55τ − ° ° − ° °A A A

120 cos 55 sin 55τ = ° ° 56.4 MPaτ =

Page 3: Mechanics of Materials

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PROBLEM 7.5

For the given state of stress, determine (a) the principal planes, (b) the principal stresses.

SOLUTION

60 MPa 40 MPa 35 MPax y xyσ σ τ= − = − =

(a) 2 (2) (35)

tan 2 3.5060 40

xyp

x y

τθ

σ σ= = = −

− − +

2 74.05pθ = − ° 37.0 , 53.0pθ = − ° °

(b)

2

2max, min

22

2 2

60 40 60 40(35)

2 2

50 36.4 MPa

x y x yxy

σ σ σ σσ τ

+ − = ± +

− − − + = ± +

= − ±

max 13.60 MPaσ = −

min 86.4 MPaσ = −

Page 4: Mechanics of Materials

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PROBLEM 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

8 ksi 12 ksi 5 ksix y xyσ σ τ= − = =

(a) 8 12

tan 2 2.02 2(5)x y

sxy

σ σθ

τ− − −= − = − = +

2 63.435sθ = ° 31.7 , 121.7sθ = ° °

(b) 2

2max 2

x yxy

σ στ τ

− = +

2

28 12(5)

2

− − = +

max 11.18 ksiτ =

(c) ave 2

σ σσ σ

+′ = = x y

8 12

2

− += 2.00 ksiσ′ =

Page 5: Mechanics of Materials

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PROBLEM 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

0 80 MPa 50 MPa

40 MPa 40 MPa2 2

cos 2 sin 22 2

sin 2 + cos 22

cos 2 sin 22 2

x y xy

x y x y

x y x yx xy

x yx y xy

x y x yy xy

σ σ τσ σ σ σ

σ σ σ σσ θ τ θ

σ στ θ τ θ

σ σ σ σσ θ τ θ

′ ′

= = − = −

+ −= − =

+ −= + +

−= −

+ −= − −

(a) 25θ = − ° 2 50θ = − °

40 40 cos ( 50 ) 50 sin ( 50°)xσ ′ = − + − ° − − 24.0 MPaxσ ′ =

40 sin ( 50°) 50 cos ( 50 )x yτ ′ ′ = − − − − ° 1.5 MPax yτ ′ ′ = −

40 40 cos ( 50 ) 50 sin ( 50 )yσ ′ = − − − ° + − ° 104.0 MPayσ ′ = −

(b) 10 2 20θ θ= ° = °

40 40 cos (20°) 50 sin (20°)xσ ′ = − + − 19.5 MPaxσ ′ = −

40 sin (20°) 50 cos (20°)x yτ ′ ′ = − − 60.7 MPax yτ ′ ′ = −

40 40 cos (20°) + 50 sin (20°)yσ ′ = − − 60.5 MPayσ ′ = −

Page 6: Mechanics of Materials

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PROBLEM 7.20

Two members of uniform cross section 50 80 mm× are glued together along plane a-a that forms an angle of 25° with the horizontal. Knowing that the allowable stresses for the glued joint are 800 kPaσ = and 600 kPa,τ = determine the largest centric load P that can be applied.

SOLUTION

For plane a-a, 65 .θ = °

2 2 2

3 3 33

2 2

2 2

3

0, 0,

cos sin 2 sin cos 0 sin 65 0

(50 10 )(80 10 )(800 10 )3.90 10 N

sin 65 sin 65

( )sin cos (cos sin ) sin 65 cos65 0

(50 10 )(8

sin 65 cos 65

x xy y

x y xy

x y xy

P

AP

A

AP

P

A

AP

σ τ σ

σ σ θ σ θ τ θ θ

σ

τ σ σ θ θ τ θ θ

τ

− −

= = =

= + + = + ° +

× × ×= = = ×° °

= − − + − = ° ° +

×= =° °

3 330 10 )(600 10 )

6.27 10 Nsin 65 cos65

−× × = ×° °

Allowable value of P is the smaller one. 3.90 kNP =

Page 7: Mechanics of Materials

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PROBLEM 7.26

The axle of an automobile is acted upon by the forces and couple shown. Knowing that the diameter of the solid axle is 32 mm, determine (a) the principal planes and principal stresses at point H located on top of the axle, (b) the maximum shearing stress at the same point.

SOLUTION

31 1(32) 16 mm 16 10 m

2 2c d −= = = = ×

Torsion: 63 3 3

2 2(350 N m)54.399 10 Pa 54.399 MPa

(16 10 m)

Tc T

J cτ

π π −⋅= = = = × =

×

Bending: 4 3 4 9 4

3

36

9

(16 10 ) 51.472 10 m4 4

(0.15m)(3 10 N) 450 N m

(450)(16 10 )139.882 10 Pa 139.882 MPa

51.472 10

I c

M

My

I

π π

σ

− −

= = × = ×

= × = ⋅

×= − = − = − × = −×

Top view: Stresses:

ave

22 2 2

139.882 MPa 0 54.399 MPa

1 1( ) ( 139.882 0) 69.941 MPa

2 2

( 69.941) ( 54.399) 88.606 MPa2

x y xy

x y

x yxyR

σ σ τ

σ σ σ

σ στ

= − = = −

= + = − + = −

− = + = − + − =

(a) max ave 69.941 88.606Rσ σ= + = − + max 18.67 MPaσ =

min ave 69.941 88.606Rσ σ= − = − − min 158.5 MPaσ = −

Page 8: Mechanics of Materials

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PROBLEM 7.26 (Continued)

2 (2)( 54.399)

tan 2 0.77778 2 37.88139.882

xyp p

x y

τθ θ

σ σ−= = = = °

− −

18.9 and 108.9°pθ = °

(b) max 88.6 MPaRτ = = max 88.6 MPaτ =

Page 9: Mechanics of Materials

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PROBLEM 7.32

Solve Probs 7.7 and 7.11, 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

ave

4 ksi,

12 ksi,

15 ksi

4 ksi2

x

y

xy

x y

σστ

σ σσ

== −

= −

+= = −

Plotted points for Mohr’s circle:

ave

: ( , ) (4 ksi, 15 ksi)

: ( , ) ( 12 ksi, 15 ksi)

: ( , 0) ( 4 ksi, 0)

x xy

y xy

X

Y

C

σ τσ τσ

− =

= − −

= −

(a) 15

tan 1.8758

FX

CFα = = =

61.93

130.96

2a

α

θ α

= °

= − = − ° 31.0aθ = − °

180 118.07

159.04

2b

β α

θ β

= ° − = °

= = ° 59.0bθ = °

2 2 2 2( ) ( ) (8) (15) 17 ksiR CF FX= + = + =

(b) max ave 4 17a Rσ σ σ= = + = − + max 13.00 ksiσ =

min min ave 4 17Rσ σ σ= = − = − − min 21.0 ksiσ = −

(a′) 45 14.04d aθ θ= + ° = ° 14.0dθ = °

45 104.04e bθ θ= + ° = ° 104.0eθ = °

max Rτ = max 17.00 ksiτ =

(b′) aveσ σ′ = 4.00 ksiσ ′ = −

Page 10: Mechanics of Materials

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PROBLEM 7.41

Solve Prob. 7.19, using Mohr’s circle.

PROBLEM 7.19 A steel pipe of 12-in. outer diameter is fabricated from 14 -in.-thick plate by welding along a helix which 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

( )( )

2 2 2

1 2

2 2 2 2 22 1

4 4 4 4 42 1

112 in. 6 in., 0.25 in.

25.75 in.

(6 5.75 ) 9.2284 in

(6 5.75 ) 318.67 in2 2

d c d t

c c t

A c c

J c c

π π

π π

= = = =

= − =

= − = − =

= − = − =

Stresses:

2

404.3344 ksi

9.2284(80)(6)

1.5063 ksi318.67

0, 4.3344 ksi, 1.5063 ksix y xy

P

ATc

J

σ

τ

σ σ τ

= − = − = −

= − = − =

= = − =

Draw the Mohr’s circle.

: (0, 1.5063 ksi)

: ( 4.3344 ksi,1.5063 ksi)

: ( 2.1672 ksi, 0)

X

Y

C

−−−

2 2

1.5063tan 0.69504 34.8

2.1672(2)(22.5 ) 10.8

(2.1672) (1.5063) 2.6393 ksiR

α α

β α

= = = °

= ° − = °

= + =

2.1672 2.6393 cos 10.8wσ = − − ° 4.76 ksiwσ = −

2.6393sin10.2wτ = − ° 0.467 ksiwτ = −

Page 11: Mechanics of Materials

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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

3

63 3

100 10125 10 Pa 125 MPa

(10 10 )(80 10 )x

P

Aσ − −

×= = = × =× ×

0 0y xyσ τ= =

From Mohr’s circle:

(a) 30

sin 2 0.4862.5

β = = 14.3β = °

(b) 62.5 62.5cos 2σ β= +

117.3 MPaσ =

Page 12: Mechanics of Materials

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PROBLEM 7.45

Solve Prob. 7.23, using Mohr’s circle.

PROBLEM 7.23 A 400-lb vertical force is applied at D to a gear attached to the solid 1-in.-diameter shaft AB. Determine the principal stresses and the maximum shearing stress at point H located as shown on top of the shaft.

SOLUTION

Equivalent force-couple system at center of shaft in section at point H:

400 lb (400)(6) 2400 lb inV M= = = ⋅

(400)(2) 800 lb inT = = ⋅

Shaft cross section 1

1 in. 0.5 in.2

d c d= = =

4 4 410.098175 in 0.049087 in

2 2J c I J

π= = = =

Torsion: 3(800)(0.5)4.074 10 psi 4.074 ksi

0.098175

Tc

Jτ = = = × =

Bending: 3(2400)(0.5)24.446 10 psi 24.446 ksi

0.049087

Mc

Iσ = = = × =

Transverse shear: Stress at point H is zero.

Resultant stresses:

ave

22

2 2

24.446 ksi, 0, 4.074 ksi

1( ) 12.223 ksi

2

2

(12.223) (4.074) 12.884 ksi

x y xy

x y

x yxyR

σ σ τ

σ σ σ

σ στ

= = =

= + =

− = +

= + =

avea Rσ σ= + 25.107 ksiaσ =

aveb Rσ σ= − 0.661 ksibσ = −

max Rτ = max 12.88 ksiτ =

Page 13: Mechanics of Materials

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PROBLEM 7.47

Solve Prob. 7.25, using Mohr’s circle.

PROBLEM 7.25 The steel pipe AB has a 102-mm outer diameter and a 6-mm wall thickness. Knowing that arm CD is rigidly attached to the pipe, determine the principal stresses and the maximum shearing stress at point K.

SOLUTION

102

51 mm 45 mm2 2o

o i od

r r r t= = = = − =

( )4 4 6 4 6 44.1855 10 mm 4.1855 10 m2 o iJ r rπ −= − = × = ×

6 412.0927 10 m

2I J −= = ×

Force-couple system at center of tube in the plane containing points H and K:

3

3 3

3 3

10 10 N

(10 10 )(200 10 ) 2000 N m

(10 10 )(150 10 ) 1500 N m

x

y

z

F

M

M

= ×

= × × = ⋅

= − × × = − ⋅

Torsion:

3

3

6

2000 N m

51 10 m

(2000)(51 10 )24.37 MPa

4.1855 10

y

o

xy

T M

c r

Tc

= = ⋅

= = ×

×= = =×

Note that the local x-axis is taken along a negative global z-direction.

Transverse shear: Stress due to xV F= is zero at point K.

Bending: 3

6

(1500)(51 10 )36.56 MPa

2.0927 10z

y

M c

−×= = =

×

Point K lies on compression side of neutral axis. 36.56 MPayσ = −

Page 14: Mechanics of Materials

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PROBLEM 7.47 (Continued)

Total stresses at point K: 0, 36.56 MPa, 24.37 MPax y xyσ σ τ= = − =

ave1

( ) 18.28 MPa2 x yσ σ σ= + = −

2

2 30.46 MPa2

x yxyR

σ στ

− = + =

max ave 18.28 30.46Rσ σ= + = − +

max 12.18 MPaσ =

min ave 18.28 30.46Rσ σ= − = − −

min 48.74 MPaσ = −

max Rτ = max 30.46 MPaτ =

Page 15: Mechanics of Materials

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PROBLEM 7.61

For the element shown, determine the range of values of xyτ for which the maximum tensile stress is equal to or less than 60 MPa.

SOLUTION

ave

20 MPa 120 MPa

1( ) 70 MPa

2

x y

x y

σ σ

σ σ σ

= − = −

= + = −

Set max ave

max ave

60 MPa

130 MPa

R

R

σ σσ σ

= = += − =

But

2

2

22

2 2

2

2

130 50

120 MPa

x xxy

x xxy

R

R

σ σ τ

σ στ

− = +

− = −

= −=

Range of :xyτ 120 MPa 120 MPaxyτ− ≤ ≤

Page 16: Mechanics of Materials

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PROBLEM 7.66

For the state of plane stress shown, determine the maximum shearing stress when (a) 6 ksixσ = and 18 ksiyσ = , (b) 14 ksixσ = and

2 ksiyσ = . (Hint: Consider both in-plane and out-of-plane shearing stresses.)

SOLUTION

(a)

ave

6ksi, 18 ksi, 8 ksi

1( ) 12 ksi

2

x y xy

x y

σ σ τ

σ σ σ

= = =

= + =

22

2 2

2

6 8 10 ksi

x yxyR

σ στ

− = +

= + =

ave

ave

12 10 22 ksi (max)

12 10 2 ksi

0 (min)

a

b

c

R

R

σ σσ σσ

= + = + == − = − ==

max(in-plane) 10 ksiRτ = =

max max min1

( )2

τ σ σ= − max 11 ksiτ =

(b)

22

2 2

14 ksi, 2 ksi, 8 ksi

1( ) 8 ksi

2

2

6 8 10 ksi

x y xy

a x y

x yxyR

σ σ τ

σ σ σ

σ στ

= = =

= + =

− = +

= + =

ave

ave

18 ksi (max)

2 ksi (min)

0

a

b

c

R

R

σ σσ σσ

= + == − = −=

max

min

max max min

18 ksi

2 ksi

1( )

2

σσ

τ σ σ

== −

= − max 10 ksiτ =

Page 17: Mechanics of Materials

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PROBLEM 7.72

For the state of stress shown, determine the maximum shearing stress when (a) 0,zσ = (b) 45zσ = + MPa, (c) 45 MPa.zσ = −

SOLUTION

100 MPa, 20 MPa, 75 MPax y xyσ σ τ= = =

ave

2

2

2 2

ave

ave

1( ) 60 MPa

2

2

40 75 85 MPa

145 MPa

25 MPa

x y

x yxy

a

b

R

R

R

σ σ σ

σ στ

σ σσ σ

= + =

− = +

= + == + == − = −

(a) 0, 145 MPa, 25 MPaz a bσ σ σ= = = −

max min max max min1

145 MPa, 25 MPa, ( )2

σ σ τ σ σ= = − = − max 85 MPaτ =

(b) 45 MPa, 145 MPa, 25 MPaz a bσ σ σ= + = = −

max min145 MPa, 25 MPa,σ σ= = − max max min1

( )2

τ σ σ= − max 85 MPaτ =

(c) 45 MPa, 145 MPa, 25 MPaz a bσ σ σ= − = = −

max 145 MPa,σ = min 45 MPa,σ = − max max min1

( )2

τ σ σ= − max 95 MPaτ =

Page 18: Mechanics of Materials

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PROBLEM 7.83

The state of plane stress shown occurs in a machine component made of a steel with 45 ksi.Yσ = Using the maximum-distortion-energy criterion, determine whether

yield will occur when (a) 9 ksi,xyτ = (b) 18 ksi,xyτ = (c) 20 ksi.xyτ = If yield

does not occur, determine the corresponding factor of safety.

SOLUTION

36 ksi, 21 ksi, 0x y zσ σ σ= = =

For stresses in xy-plane, ave1

( ) 28.5 ksi2 x yσ σ σ= + =

7.5 ksi2

x yσ σ−=

(a) 2

2 2 2

ave ave

9 ksi (7.5) (9) 11.715 ksi2

40.215 ksi, 16.875 ksi

x yxy xy

a b

R

R R

σ στ τ

σ σ σ σ

− = = + = + =

= + = = − =

2 2 34.977 ksi 45 ksia b a bσ σ σ σ+ − = < (No yielding)

45

. .39.977

F S = . . 1.287F S =

(b) 2

2 2 2

ave ave

18 ksi (7.5) (18) 19.5 ksi2

48 ksi, 9 ksi

x yxy xy

a b

R

R R

σ στ τ

σ σ σ σ

− = = + = + =

= + = = − =

2 2 44.193 ksi 45 ksia b a bσ σ σ σ+ − = < (No yielding)

45

. .44.193

F S = . . 1.018F S =

(c) 2

2 2 2

ave ave

20 ksi (7.5) (20) 21.36 ksi2

49.86 ksi, 7.14 ksi

x yxy xy

a b

R

R R

σ στ τ

σ σ σ σ

− = = + = + =

= + = = − =

2 2 46.732 ksi 45 ksia b a bσ σ σ σ+ − = > (Yielding occurs)

Page 19: Mechanics of Materials

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PROBLEM 7.84

Solve Prob. 7.83, using the maximum-shearing-stress criterion.

PROBLEM 7.83 The state of plane stress shown occurs in a machine component made of a steel with 45 ksi.Yσ = Using the maximum-distortion-energy criterion, determine whether yield will occur when (a) 9 ksi,xyτ = (b) 18 ksi,xyτ = (c)

20 ksi.xyτ = If yield does not occur, determine the corresponding factor of safety.

SOLUTION

36 ksi, 21 ksi, 0x y zσ σ σ= = =

For stress in xy-plane, ave1

( ) 28.5 ksi 7.5 ksi2 2

x yx y

σ σσ σ σ

−= + = =

(a) 2

2

ave ave

max min34.977 ksi,

9 ksi 11.715 ksi2

40.215 ksi, 16.875 ksi

0

x yxy xy

a b

R

R R

τ σ

σ στ τ

σ σ σ σ

− = = + =

= + = = − == =

max max min2 40.215 ksi 45 ksiτ σ σ= − = < (No yielding)

45

. .40.215

F S = . . 1.119F S =

(b)

max

22

ave ave

min48 ksi

18 ksi 19.5 ksi2

48 ksi, 9 ksi

0

x yxy xy

a b

R

R R

σ

σ στ τ

σ σ σ σσ

− = = + =

= + = = − == =

max max min2 48 ksi 45 ksiτ σ σ= − = > (Yielding occurs)

(c)

max

22

ave ave

min49.86 ksi

20 ksi 21.36 ksi2

49.86 ksi 7.14 ksi

0

x yxy xy

a b

R

R R

τ σ

σ στ τ

σ σ σ σ

− = = + =

= + = = − == =

max max min2 49.86 ksi 45 ksiτ σ σ= − = > (Yielding occurs)

Page 20: Mechanics of Materials

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PROBLEM 7.85

The 36-mm-diameter shaft is made of a grade of steel with a 250-MPa tensile yield stress. Using the maximum-shearing-stress criterion, determine the magnitude of the torque T for which yield occurs when 200 kN.P =

SOLUTION

3 3

2 3 2 3 2

36

3

ave

1200 kN 200 10 N 18 mm 18 10 m

2

(18 10 ) 1.01788 10 m

200 10196.488 10 Pa

1.01788 10196.488 MPa

1 10 ( ) 98.244 MPa

2 2

y

x x y y

P c d

A c

P

A

π π

σ

σ σ σ σ σ

− −

= = × = = = ×

= = × = ×

×= − = − = ××

=

= = + = =

22 2 2

ave

ave

(98.244)2

(positive)

(negative)

2

x yxy xy

a

b

a b a b a a b b

R

R

R

R

σ στ τ

σ σσ σσ σ σ σ σ σ σ σ

− = + = +

= += −

− = − > − >

Maximum shear stress criterion under the above conditions:

2 250 MPa 125 MPaa b YR Rσ σ σ− = = = =

Equating expressions for R,

2 2

2 2 6

125 (98.244)

(125) (98.244) 77.286 MPa 77.286 10 Pa

xy

xy

τ

τ

= +

= − = = ×

Torsion: 4 3 4 9 4(18 10 ) 164.896 10 m2 2

xy

J c

Tc

J

π π

τ

− −= = × = ×

=

9 6

3

(164.846 10 )(77.286 10 )

18 10708 N m

xyJT

c

τ −

−× ×= =

×= ⋅ 708 N mT = ⋅

Page 21: Mechanics of Materials

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PROBLEM 7.86

Solve Prob. 7.85, using the maximum-distortion-energy criterion.

PROBLEM 7.85 The 36-mm-diameter shaft is made of a grade of steel with a 250-MPa tensile yield stress. Using the maximum-shearing-stress criterion, determine the magnitude of the torque T for which yield occurs when 200 kN.P =

SOLUTION

3 3

2 3 2 3 2

36

3

ave

1200 kN 200 10 N 18 mm 18 10 m

2

(18 10 ) 1.01788 10 m

200 10196.488 10 Pa

1.01788 10196.448 MPa

1 10 ( ) 98.244 MPa

2 2

y

x x y y

P c d

A c

P

A

π π

σ

σ σ σ σ σ

− −

= = × = = = ×

= = × = ×

×= − = − = ××

=

= = + = =

2

2 2 2

ave ave

(98.244)2

x yxy xy

a b

R

R R

σ στ τ

σ σ σ σ

− = + = +

= + = −

Distortion energy criterion:

2 2 2

2 2 2ave ave ave ave

2 2 2ave

2 2 2 2

( ) ( ) ( )( )

3

(98.244) (3)[(98.244) ] (250)

89.242 MPa

a b a b Y

Y

Y

xy

xy

R R R R

R

σ σ σ σ σ

σ σ σ σ σ

σ σ

ττ

+ − =

+ + − − + − =

+ =

+ + =

= ±

Torsion: 4 3 4 9 4(18 10 ) 164.846 10 m2 2

xy

J c

Tc

J

π π

τ

− −= = × = ×

=

9 6

3

(164.846 10 )(89.242 10 )

18 10818 N m

xyJT

c

τ −

−× ×= =

×= ⋅ 818 N mT = ⋅

Page 22: Mechanics of Materials

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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

36

5 m 6 mm 0.006 m, 2.494 m2

(350 10 Pa)(2.494 m)72.742 10 Pa

2 2(0.006 m)

dd t r t

pr

= = = = − =

×= = = ×

72.7 MPaσ =

max

min

72.742 MPa

0 (Neglectingsmall radialstress)

σσ

=≈

max max min1

( )2

τ σ σ= − max 36.4 MPaτ =

Page 23: Mechanics of Materials

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PROBLEM 7.104

A steel penstock has a 750-mm outer diameter, a 12-mm wall thickness, and connects a reservoir at A with a generating station at B. Knowing that the density of water is 31000 kg/m , determine the maximum normal stress and the maximum shearing stress in the penstock under static conditions.

SOLUTION

3

3

3 2

6

6 36

1 3

1 1(750) 12 363 mm 363 10 m

2 2

12 mm 12 10 m

(1000 kg/m )(9.81 m/s )(300 m)

2.943 10 Pa

(2.943 10 )(363 10 )89.0 10 Pa

12 10

r d t

t

p gh

pr

t

ρ

σ

= − = − = = ×

= = ×

= =

= ×

× ×= = = ××

max 1σ σ= max 89.0 MPaσ =

min 0pσ = − ≈

max max min1

( )2

τ σ σ= − max 44.5 MPaτ =

Page 24: Mechanics of Materials

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PROBLEM 7.114

For the tank of Prob. 7.112, determine the range of values of β that can be used if the shearing stress parallel to the weld is not to exceed 12 MPa when the gage pressure is 600 kPa.

PROBLEM 7.112 The pressure tank shown has a 8-mm wall thickness and butt-welded seams forming an angle 20β = ° with a transverse plane. For a gage pressure of 600 kPa, determine (a) the normal stress perpendicular to the weld, (b) the shearing stress parallel to the weld.

SOLUTION

3 11.6 m 8 10 mm 0.792 m

2d t r d t−= = × = − =

3

1 3

6

2

1 2

(600 10 )(0.792)

8 10

59.4 10 Pa = 59.4 MPa

29.7 MPa2

14.85 MPa2

|sin 2 |w

pr

t

pr

t

R

R

σ

σ

σ σ

τ β

−×= =

×= ×

= =

−= =

=

12

|sin 2 | 0.8080814.85

Na R

τβ = = =

2 53.91aβ = − ° 27.0aβ = + °

2 53.91bβ = + ° 27.0bβ = °

2 180 53.91 126.09cβ = ° − ° = + ° 63.0β = °c

2 180 53.91 233.91dβ = ° + ° = + ° 117.0dβ = °

Let the total range of values for β be 180 < 180β− ° ≤ °

Safe ranges for β: 22.0 27.0°β− °≤ ≤

and 63.0 117.0°β°≤ ≤

Page 25: Mechanics of Materials

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PROBLEM 7.116

The pressurized tank shown was fabricated by welding strips of plate along a helix forming an angle β with a transverse plane. Determine the largest value of β that can be used if the normal stress perpendicular to the weld is not to be larger than 85 percent of the maximum stress in the tank.

SOLUTION

1 2 2

pr pr

t tσ σ= =

ave 1 2

1 2

ave

1 3( )

2 41

2 4cos 2w

pr

tpr

Rt

R

σ σ σ

σ σ

σ σ β

= + =

−= =

= −

3 1

0.85 cos 24 4

pr pr

t tβ = −

3cos 2 4 0.85 0.4

4

2 113.6

β

β

= − − = −

= ° 56.8β = °

Page 26: Mechanics of Materials

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PROBLEM 7.124

A pressure vessel of 10-in. inner diameter and 0.25-in. wall thickness is fabricated from a 4-ft section of spirally-welded pipe AB and is equipped with two rigid end plates. The gage pressure inside the vessel is 300 psi and 10-kip centric axial forces P and P′ are applied to the end plates. Determine (a) the normal stress perpendicular to the weld, (b) the shearing stress parallel to the weld.

SOLUTION

( )

1

2

0

2 2 2 2 20

3

1 1(10) 5 in. 0.25 in.

2 2(300) (5)

6000 psi 6 ksi0.25

(300)(5)3000 psi 3 ksi

2 (2)(0.25)

5 0.25 5.25 in.

(5.25 5.00 ) 8.0503 in

10 101242 psi 1.242 ksi

8.0803

σ

σ

π π

σ

= = = =

= = = =

= = = =

= + = + =

= − = − =

×= − = − = − = −

r d t

pr

tpr

t

r r t

A r r

P

A

Total stresses. Longitudinal: 3 1.242 1.758 ksixσ = − =

Circumferential: 6 ksiyσ =

Shear: 0xyτ =

Plotted points for Mohr’s circle:

: (1.758, 0)

: (6, 0)

: (3.879)

X

Y

C

ave

2

2

2

1( ) 3.879 ksi

2

2

(1.758 6)0 2.121 ksi

2

x y

x yxyR

σ σ σ

σ στ

= + =

− = +

− = + =

(a) ave cos 70 3.879 2.121 cos 70x Rσ σ′ = + ° = − ° 3.15 ksixσ ′ =

(b) | | sin 70 2.121 sin 70xy Rτ = ° = ° | | 1.993 ksix yτ ′ ′ =

Page 27: Mechanics of Materials

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PROBLEM 7.128

For the given state of plane strain, use the method of Sec. 7.10 to determine the state of plane strain associated with axes x′ and y′ rotated through the given angle θ .

500 , 250 , 0, 15x y xyε μ ε μ γ θ= − = + = = °

SOLUTION

15θ = + °

125 375 02 2 2

cos 2 sin 22 2 2

125 ( 375 )cos30 0

x y x y xy

x y x y xyx

ε ε ε ε γμ μ

ε ε ε ε γε θ θ

μ μ

+ −= − = − =

+ −= + +

= − + − ° + 450xε μ′ = −

cos 2 sin 22 2 2

125 ( 375 )cos 30 0

x y x y xyy

ε ε ε ε γε θ θ

μ μ

′+ −

= − −

= − − − ° − 200yε μ′ =

( )sin 2 cos 2

( 500 250 )sin 30 0

x y x y xyγ ε ε θ γ θμ μ

′ ′ = − − +

= − − − ° + 375x yγ μ′ ′ =

Page 28: Mechanics of Materials

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PROBLEM 7.136

The following state of strain has been measured on the surface of a thin plate. Knowing that the surface of the plate is unstressed, determine (a) the direction and magnitude of the principal strains, (b) the maximum in-plane shearing strain, (c) the maximum shearing strain. (Use 1

3 .v = )

260 , 60 , 480x y xyε μ ε μ γ μ= − = − = +

SOLUTION

For Mohr’s circle of strain, plot points:

: ( 260 , 240 )

: ( 60 , 240 )

: ( 160 , 0)

X

Y

C

μ μμ μ

μ

− −−−

480

tan 2 2.4260 60

xyp

x y

γθ

ε ε= = = −

− − +

2 67.38pθ = − ° 33.67bθ = − °

56.31aθ = °

2 2(100 ) (240 )

260

R

R

μ μμ

= +=

(a) ave 160 260a Rε ε μ μ= + = − + 100aε μ=

ave 160 260b Rε ε μ μ= − = − − 420bε μ= −

(b) max(in-plane) max(in-plane)1

22

R Rγ γ= = max (in-plane) 520γ μ=

1/3

( ) ( ) ( 260 60)1 1 2/3

160

c a b x yv v

v vε ε ε ε ε

μ

= − + = − + = − − −− −

=

max min160 420ε μ ε μ= = −

(c) max max min 160 420γ ε ε μ μ= − = + max 580γ μ=

Page 29: Mechanics of Materials

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PROBLEM 7.140

For the given state of plane strain, use Mohr’s circle to determine (a) the orientation and magnitude of the principal strains, (b) the maximum in-plane shearing strain, (c) the maximum shearing strain.

60 , 240 , 50x y xyε μ ε μ γ μ= + = + = −

SOLUTION

Plotted points:

: (60 , 25 )

: (240 , 25 )

: (150 , 0)

X

Y

C

μ μμ μμ

50

tan 2 0.27777860 240

xyp

x y

γθ

ε ε−= = =

− −

2 15.52pθ = ° 97.76aθ = °

7.76bθ = °

2 2(90 ) (25 ) 93.4R μ μ μ= + =

(a) ave 150 93.4a Rε ε μ μ= + = + 243.4aε μ=

ave 150 93.4b Rε ε μ μ= − = − 56.6bε μ=

(b) max (in-plane) 2Rγ = max (in-plane) 186.8γ μ=

(c) max min0, 243.4 , 0cε ε μ ε= = =

max max minγ ε ε= − max 243.4γ =

Page 30: Mechanics of Materials

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PROBLEM 7.147

The strains determined by the use of the rosette attached as shown during the test of a machine element are

61

62

63

93.1 10 in./in.

385 10 in./in.

210 10 in./in.

ε

ε

ε

= − ×

= + ×

= + ×

Determine (a) the orientation and magnitude of the principal strains in the plane of the rosette, (b) the maximum in-plane shearing strain.

SOLUTION

Use 1 1

( ) ( )cos 2 sin 22 2 2

xyx x y x y

γε ε ε ε ε θ θ′ = + + − +

where 75θ = − ° for gage 1,

0θ = for gage 2,

and 75θ = + ° for gage 3.

11 1

( ) ( )cos ( 150 ) sin ( 150 )2 2 2

xyx y x y

γε ε ε ε ε= + + − − ° + − ° (1)

21 1

( ) ( )cos 0 sin 02 2 2

xyx y x y

γε ε ε ε ε= + + − + (2)

31 1

( ) ( )cos (150 ) sin (150 )2 2 2

xyx y x y

γε ε ε ε ε= + + − ° + ° (3)

From Eq. (2), 6385 10 in/inx zε ε −= = ×

Adding Eqs. (1) and (3),

1 3

1 3

6 6 6

6

( ) ( )cos 150

(1 cos 150 ) (1 cos 150 )

(1 cos 150 )

(1 cos 150 )

93.1 10 210 10 385 10 (1 cos 150 )

1 cos 150

35.0 10 in/in

x y x y

x y

xy

ε ε ε ε ε εε εε ε εε

− − −

+ = + + − °= + ° + − °

+ − + °=

− °− × + × − × + °=

− °= ×

Page 31: Mechanics of Materials

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PROBLEM 7.147 (Continued)

Subtracting Eq. (1) from Eq. (3),

3 1

6 63 1

6

sin 150

210 10 ( 93.1 10 )

sin 150 sin 150

606.2 10 in/in

xy

xy

ε ε γ

ε εγ− −

− = °

− × − − ×= =° °

= ×

6

6 6

606.2 10tan 2 1.732

385 10 35.0 10

xyp

x y

γθ

ε ε

− −×= = =

− × − × (a) 30.0 , 120.0a bθ θ= ° = °

6 6ave

6

2 2

2 26 66

6 6ave

1 1( ) (385 10 35.0 10 )

2 2

210 10 in/in

2 2

385 10 35.0 10 606.2350.0 10

2 2

210 10 350.0 10

x y

x y xy

a

R

R

ε ε ε

ε ε γ

ε ε

− −

− −−

− −

= + = × + ×

= ×

− = +

× − × = + = ×

= + = × + × 6560 10 in/inaε −= ×

6 6ave 210 10 350.0 10b Rε ε − −= − = × − × 6140.0 10 in/inbε −= − ×

(b) max (in-plane) 6350.0 10 in/in2

Rγ −= = × 6

max (in-plane) 700 10 in/inγ −= ×

Page 32: Mechanics of Materials

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PROBLEM 7.150

A single strain gage is cemented to a solid 4-in.-diameter steel shaft at an angle 25β = ° with a line parallel to the axis of the shaft. Knowing that

611.5 10 psi,G = × determine the torque T indicated by a gage reading of 6300 10 in./in.−×

SOLUTION

For torsion, 0

0 0

0,

1( ) 0

1( ) 0

1

2 2

x y

x x y

y y x

xy xy

vE

vE

G G

σ σ τ τ

ε σ σ

ε σ σ

τ τγ γ

= = =

= − =

= − =

= =

Draw the Mohr’s circle for strain.

0

0

2

sin 2 sin 22x

RG

RG

τ

τε β β′

=

= =

But 0 3

22

sin 2xGTc T

J c

ετβπ′= = =

3

3 6 6

sin 2

(2) (11.5 10 )(300 10 )

sin 50

xc GT

π εβ

π

=

× ×=°

3113.2 10 lb in= × ⋅ 113.2 kip inT = ⋅

Page 33: Mechanics of Materials

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PROBLEM 7.157

Solve Prob. 7.156, assuming that the rosette at point A indicates the following strains:

61

62

63

30 10 in./in.

250 10 in./in.

100 10 in./in.

ε

ε

ε

= − ×

= + ×

= + ×

PROBLEM 7.156 A centric axial force P and a horizontal force Qx are both applied at point C of the rectangular bar shown. A 45° strain rosette on the surface of the bar at point A indicates the following strains:

61

62

63

60 10 in./in.

240 10 in./in.

200 10 in./in.

ε

ε

ε

= − ×

= + ×

= + ×

Knowing that 629 10 psiE = × and 0.30,v = determine the magnitudes of P and Qx.

SOLUTION

61

63

62 1 3

2 2

2 2

3

3

30 10

100 10

2 430 10

29( ) [ 30 (0.3)(100)]

1 1 (0.3)0

29( ) [100 (0.3)( 30)]

1 1 (0.3)

2.9 10 psi

(2)(6)(2.9 10 )

x

y

xy

x x y

y y x

y y

Ev

v

Ev

v

PP A

A

ε εε ε

γ ε ε ε

σ ε ε

σ ε ε

σ σ

= = − ×= = + ×

= − − = ×

= + = − +− −

=

= + = + −− −

= ×

= = = ×

334.8 10 lb= × 34.8 kipsP =

Page 34: Mechanics of Materials

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PROBLEM 7.157 (Continued)

66

3

3 3 4

3

29 1011.1538 10 psi

2(1 ) (2)(1.30)

(11.1538)(430) 4.7962 10 psi

1 1(2)(6) 36 in

12 12ˆ (2)(3)(1.5) 9 in

2 in.

xy xy

EG

v

G

I bh

Q Ay

t

τ γ

×= = = ×+

= = = ×

= = =

= = ==

33

ˆ

(36)(2)(4.7962 10 )38.37 10 lb

ˆ 9

xy

xy

VQ

ItIt

VQ

Q V

τ

τ

=

×= = = ×

= 38.4 kipsQ =