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7/21/2019 Mechanics of Materials Solutions Chapter11 Probs18 25 http://slidepdf.com/reader/full/mechanics-of-materials-solutions-chapter11-probs18-25 1/13  Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted.  Any other reproduction or translation of this work beyond that  permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful. 11.18a For the beams and loadings shown  below, assume that  EI = 3.0 × 10 4  kN-m 2 is constant for each beam. (a) For the beam in Fig. P11.18a, determine the concentrated upward force  P  required to make the total beam deflection at  B equal to zero (i.e., v  B  = 0). Fig. P11.18a Solution Downward deflection at  B due to 15 kN/m uniformly distributed load. [Appendix C, SS beam with uniformly distributed load over portion of span.]  Relevant equation from Appendix C: 3 2 2 (4 7 3 ) 24  B wa v L aL a  LEI = +  Values: w = 15 kN/m, L = 7 m, a = 3.5 m,  EI = 3.0 × 10 4  kN-m 2  Computation: 3 2 2 3 3 2 2 (4 7 3 ) 24 (15 kN/m)(3.5 m) 234.472656 kN-m 4(7 m) 7(3.5 m)(7 m) 3(3.5 m) 24(7 m)  B wa v L aL a  LEI  EI EI = + = + =  Upward deflection at  B due to concentrated load  P . [Appendix C, SS beam with concentrated load at midspan.]  Relevant equation from Appendix C: 3 48  B  PL v  EI =  Values:  L = 7 m, EI = 3.0 × 10 4  kN-m 2  Computation: 3 3 3 (7 m) (7.145833 m) 48 48  B  PL P v  EI EI EI = = =  Compatibility equation at  B: 3 3 3 3 234.472656 kN-m (7.145833 m ) 0 234.472656 kN-m 32.8125 kN 32.8 kN 7.145833 m  P  EI EI  P + = = = =  Ans. 
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Page 1: Mechanics of Materials Solutions Chapter11 Probs18 25

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11.18a For the beams and loadings shown below, assume that EI = 3.0 × 10

4 kN-m

2is

constant for each beam.

(a) For the beam in Fig. P11.18a, determine

the concentrated upward force P  required tomake the total beam deflection at B equal to

zero (i.e., v B = 0).

Fig. P11.18a 

Solution

Downward deflection at  B due to 15 kN/m uniformly distributed load.

[Appendix C, SS beam with uniformly distributed load over portion of span.]

 Relevant equation from Appendix C:3

2 2(4 7 3 )24

 B

wav L aL a

 LEI = − − +  

Values: w = 15 kN/m, L = 7 m, a = 3.5 m,

 EI = 3.0 × 104

 kN-m2

 

Computation:3

2 2

3 32 2

(4 7 3 )24

(15 kN/m)(3.5 m) 234.472656 kN-m4(7 m) 7(3.5 m)(7 m) 3(3.5 m)

24(7 m)

 B

wav L aL a

 LEI 

 EI EI 

= − − +

⎡ ⎤= − − + = −⎣ ⎦  

Upward deflection at  B due to concentrated load  P .

[Appendix C, SS beam with concentrated load at midspan.]

 Relevant equation from Appendix C:3

48 B

 PLv

 EI =  

Values:  L = 7 m, EI = 3.0 × 10

4 kN-m

Computation:3 3 3(7 m) (7.145833 m )

48 48 B

 PL P P v

 EI EI EI = = =  

Compatibility equation at  B:3 3

3

3

234.472656 kN-m (7.145833 m )0

234.472656 kN-m32.8125 kN 32.8 kN

7.145833 m

 P 

 EI EI 

 P 

− + =

∴ = = =   Ans. 

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11.18b  For the beams and loadings shown below, assume that EI = 3.0 × 10

4 kN-m

2is

constant for each beam.

(b) For the beam in Fig. P11.18b, determinethe concentrated moment  M   required to

make the total beam slope at A equal to zero

(i.e., θ  A = 0).

Fig. P11.18b 

Solution

Slope at  A due to 32 kN concentrated load.

[Appendix C, Cantilever beam with concentrated load at tip.]

 Relevant equation from Appendix C:2

2 A

 PL

 EI θ    =   (slope magnitude)

Values:  P  = 32 kN, L = 4 m, EI = 3.0 × 10

4 kN-m

Computation:2 2 2(32 kN)(4 m) 256 kN-m

(negative slope by inspection)2 2

 A

 PL

 EI EI EI θ    = = = −  

Slope at  A due to concentrated moment  M .

[Appendix C, Cantilever beam with concentrated moment at tip.]

 Relevant equation from Appendix C:

 A  L EI 

θ    =   (slope magnitude)

Values:  L = 4 m, EI = 3.0 × 10

4 kN-m

Computation:

(4 m) (4 m)(positive slope by inspection) A

 ML M M 

 EI EI EI θ    = = =  

Compatibility equation at  A:2

2

256 kN-m (4 m)0

256 kN-m64.0 kN-m

4 m

 M 

 EI EI 

 M 

− + =

∴ = =   Ans. 

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11.19a  For the beams and loadings shown below, assume that EI = 5.0 × 10

6 kip-in.

2is

constant for each beam.

(a) For the beam in Fig. P11.19a, determinethe concentrated upward force P  required to

make the total beam deflection at B equal to

zero (i.e., v B = 0).

Fig. P11.19a 

Solution

Downward deflection at  B due to 4 kips/ft uniformly distributed load.

[Appendix C, Cantilever beam with uniformly distributed load.]

 Relevant equation from Appendix C:4

8 B

wLv

 EI = −  

Values: w = 4 kips/ft, L = 13 ft, EI = 5.0 × 10

6 kip-in.

Computation:4 4 3(4 kips/ft)(13 ft) 14,280.5 kip-ft

8 8 B

wLv

 EI EI EI = − = − = −  

Upward deflection at  B due to concentrated load  P .

[Appendix C, Cantilever beam with concentrated load at tip.]

 Relevant equation from Appendix C:3

3 B

 PLv

 EI 

=  

Values:  L = 13 ft, EI = 5.0 × 10

6 kip-in.

Computation:3 3 3(13 ft) (732.333333 ft )

3 3 B

 PL P P v

 EI EI EI = = =  

Compatibility equation at  B:3 3

3

3

14,280.5 kip-ft (732.333333 ft )0

14,280.5 kip-ft19.50 kips

732.333333 ft

 P 

 EI EI 

 P 

− + =

∴ = =   Ans. 

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11.19b  For the beams and loadings shown below, assume that EI = 5.0 × 10

6 kip-in.

2is

constant for each beam.

(b) For the beam in Fig. P11.19b, determinethe concentrated moment  M   required to

make the total beam slope at C  equal to zero

(i.e., θ C  = 0).

Fig. P11.19b 

Solution

Slope at C  due to 40-kip concentrated load.

[Appendix C, SS beam with concentrated load at midspan.]

 Relevant equation from Appendix C:2

16C 

 PL

 EI θ    =   (slope magnitude)

Values:  P  = 40 kips, L = 18 ft, EI = 5.0 × 10

6 kip-in.

Computation:2 2 2(40 kips)(18 ft) 810 kip-ft

(negative slope by inspection)16 16

 PL

 EI EI EI θ    = = =  

Slope at C  due to concentrated moment  M .

[Appendix C, SS beam with concentrated moment at one end.]

 Relevant equation from Appendix C:

3

 L

 EI 

θ    =   (slope magnitude)

Values:  L = 18 ft, EI = 5.0 × 10

6 kip-in.

Computation:

(18 ft) (6 ft)(positive slope by inspection)

3 3C 

 ML M M 

 EI EI EI θ    = = =  

Compatibility equation at C :2

2

810 kip-ft (6 ft)0

810 kip-ft135.0 kip-ft

6 ft

 M 

 EI EI 

 M 

− + =

∴ = =   Ans. 

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11.20a For the beams and loadings shown below, assume that  EI = 5.0 × 10

4 kN-m

2

is constant for each beam.

(a) For the beam in Fig. P11.20a,

determine the concentrated downwardforce  P   required to make the total beam

deflection at B equal to zero (i.e., v B = 0).

Fig. P11.20a 

Solution

Upward deflection at  B due to 105 kN-m concentrated moment.

[Appendix C, SS beam with concentrated moment at one end.]

 Relevant equation from Appendix C:

2 2(2 3 )6

 B

 M xv L Lx x

 LEI = − − +   (elastic curve)

Values:  M  = −105 kN-m, L = 8 m, x = 4 m,

 EI = 5.0 × 104 kN-m

Computation:

2 2

32 2

(2 3 )6

( 105 kN-m)(4 m) 420 kN-m2(8 m) 3(8 m)(4 m) (4 m)

6(8 m)

 B

 M xv L Lx x

 LEI 

 EI EI 

= − − +

−⎡ ⎤= − − + =⎣ ⎦  

Downward deflection at  B due to concentrated load  P .

[Appendix C, SS beam with concentrated load at midspan.]

 Relevant equation from Appendix C:3

48 B

 PLv

 EI = −  

Values:  L = 8 m, EI = 5.0 × 10

4 kN-m

Computation:3 3 3(8 m) (10.666667 m )

48 48 B

 PL P P v

 EI EI EI = − = − = −  

Compatibility equation at  B:3 3

3

3

420 kN-m (10.666667 m )0

420 kN-m39.375 kN 39.4 kN

10.666667 m

 P 

 EI EI 

 P 

− =

∴ = = =   Ans. 

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11.20b For the beams and loadings shown below, assume that  EI = 5.0 × 10

4 kN-m

2is

constant for each beam.

(b) For the beam in Fig. P11.20b, determinethe concentrated moment  M   required to

make the total beam slope at A equal to zero

(i.e., θ  A = 0).

Fig. P11.20b 

Solution

Slope at  A due to 6 kN/m uniformly distributed load.

[Appendix C, Cantilever beam with uniformly distributed load.]

 Relevant equation from Appendix C:3

6 A

wL

 EI θ    =   (slope magnitude)

Values: w = 6 kN/m, L = 5 m, EI = 5.0 × 10

4 kN-m

Computation:3 3 2(6 kN/m)(5 m) 125 kN-m

(positive slope by inspection)6 6

 A

wL

 EI EI EI θ    = = =  

Slope at  A due to concentrated moment  M .

[Appendix C, Cantilever beam with concentrated moment at tip.]

 Relevant equation from Appendix C:

 A

 L

 EI θ    =   (slope magnitude)

Values:  L = 5 m, EI = 5.0 × 10

4 kN-m

Computation:

(5 m)(negative slope by inspection) A

 ML M 

 EI EI θ    = =  

Compatibility equation at  A:2

2

125 kN-m (5 m)0

125 kN-m25.0 kN-m

5 m

 M 

 EI EI 

 M 

− =

∴ = =   Ans. 

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11.21a For the beams and loadings shown below, assume that EI = 8.0 × 10

6 kip-in.

2

is constant for each beam.

(a) For the beam in Fig. P11.21a,determine the concentrated downward

force  P   required to make the total beam

deflection at B equal to zero (i.e., v B = 0).

  Fig. P11.21a 

Solution

Upward deflection at  B due to 125 kip-ft concentrated moment.

[Appendix C, Cantilever beam with concentrated moment at tip.]

 Relevant equation from Appendix C:2

2 B

 Lv

 EI = −  

Values:  M  = −125 kip-ft, L = 15 ft, EI = 8.0 × 10

6 kip-in.

2

 Computation:2 2 3( 125 kip-ft)(15 ft) 14,062.5 kip-ft

2 2 B

 MLv

 EI EI EI 

−= − = − =  

Downward deflection at  B due to concentrated load  P .

[Appendix C, Cantilever beam with concentrated load at tip.]

 Relevant equation from Appendix C:3

3 B

 PLv

 EI = −  

Values:  L = 15 ft, EI = 8.0 × 106 kip-in.

Computation:3 3 3(15 ft) (1,125 ft )

3 3 B

 PL P P v

 EI EI EI = − = − = −  

Compatibility equation at  B:3 3

3

3

14,062.5 kip-ft (1,125 ft )0

14,062.5 kip-ft12.50 kips

1,125 ft

 P 

 EI EI 

 P 

− =

∴ = =   Ans. 

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11.21b For the beams and loadings shown below, assume that  EI = 8.0 × 10

6 kip-in.

2

is constant for each beam.

(b) For the beam in Fig. P11.21b,determine the concentrated moment

required to make the total beam slope at  A

equal to zero (i.e., θ  A = 0).

Fig. P11.21b 

Solution

Slope at  A due to 7 kips/ft uniformly distributed load.

[Appendix C, SS beam with uniformly distributed load over portion of span.]

 Relevant equation from Appendix C:2

2 2(2 )24

 A

wa L a

 LEI θ    = −   (slope magnitude)

Values: w = 7 kips/ft, L = 23 ft, a = 15 ft,

 EI = 8.0 × 106 kip-in.

Computation:2

2 2

22 2

2

(2 )24

(7 kips/ft)(15 ft)2(23 ft) (15 ft)

24(23 ft)

2,376.766304 kip-ft(negative slope by inspection)

 A

wa L a

 LEI 

 EI 

 EI 

θ    = −

⎡ ⎤= −⎣ ⎦

= −  

Slope at  A due to concentrated moment  M .[Appendix C, SS beam with concentrated moment at one end.]

 Relevant equation from Appendix C:

3 A

 L

 EI θ    =   (slope magnitude)

Values:  L = 23 ft, EI = 8.0 × 10

6 kip-in.

Computation:

(23 ft) (7.666667 ft)(positive slope by inspection)

3 3 A

 ML M M 

 EI EI EI θ    = = =  

Compatibility equation at  A:2

2

2,376.766304 kip-ft (7.666667 ft)0

2,376.766304 kip-ft310 kip-ft

7.666667 ft

 M 

 EI EI 

 M 

− + =

∴ = =   Ans. 

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11.22 For the beam and loading shown below, derive an expression for the reactions

at supports  A  and  B. Assume that  EI is

constant for the beam.

Fig. P11.22

Solution

Choose the reaction force at B as the redundant; therefore, the released beam is a cantilever.

Consider downward deflection of cantilever beam at  B due to concentrated moment  M 0.

[Appendix C, Cantilever beam with concentrated moment at tip.]

 Relevant equation from Appendix C:2 2

0

2 2 B

 L M Lv

 EI EI = − = −  

Consider upward deflection of cantilever beam at  B due to concentrated load  R B.

[Appendix C, Cantilever beam with concentrated load at tip.]

 Relevant equation from Appendix C:3 3

3 3

 B B

 PL R Lv

 EI EI = =  

Compatibility equation for deflection at  B:2 3

0 030

2 3 2

 B B

 M L R L M  R

 EI EI L− + = ∴ = ↑   Ans.

Equilibrium equations

for entire beam:

0 03 30

2 2 y A B A B

 M M  F R R R R

 L LΣ = + = ∴ = − = − = ↓   Ans. 

0 0 A A B M M M R LΣ = − − + =  

0 0 00 0 0

3 3( ) (cw)

2 2 2 A B

 M M M  M R L M L M M 

 L∴ = − = − = − =   Ans. 

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11.23 For the beam and loading shown below, derive an expression for the reactions

at supports  A  and  B. Assume that  EI is

constant for the beam.

Fig. P11.23

Solution

Choose the reaction force at B as the redundant; therefore, the released beam is a cantilever.

Consider downward deflection of cantilever beam at  B due to linearly distributed load.

[Appendix C, Cantilever beam with linearly distributed load.]

 Relevant equation from Appendix C:4

0

30 B

w Lv

 EI = −  

Consider upward deflection of cantilever beam at  B due to concentrated load  R B.

[Appendix C, Cantilever beam with concentrated load at tip.]

 Relevant equation from Appendix C:3 3

3 3

 B B

 PL R Lv

 EI EI = =  

Compatibility equation for deflection at  B:4 3

0 0030 3 10

 B B

w L R L w L R

 EI EI − + = ∴ = ↑   Ans. 

Equilibrium equations for entire beam:

0 0 0 0 04 20

2 2 10 10 5

 y A B A

w L w L w L w L w L F R R RΣ = + − = ∴ = − = = ↑   Ans.

  0 02 3

 A A B

w L L M M R L

⎛ ⎞Σ = − − + =⎜ ⎟

⎝ ⎠ 

2 2 2 2

0 0 0 0 0( ) (ccw)6 10 6 15 15

 A B

w L w L w L w L w L M R L L∴ = − = − = − =   Ans.

 

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11.24 For the beam and loading shown below,derive an expression for the reactions at

supports  A  and  B. Assume that  EI is constant

for the beam.

Fig. P11.24

Solution

Choose the reaction force at A as the redundant; therefore, the released beam is a cantilever.

Consider downward deflection of cantilever beam at  A due to concentrated load  P .

[Appendix C, Cantilever beam with concentrated load at tip.]

 Relevant equation from Appendix C:2

(3 )6

 A

 Pxv L x

 EI = − −   (elastic curve)

2 3

3Let ,2

( ) 3 73

6 2 12 A

 L x L L

 P L L PLv L

 EI EI 

= =

⎡ ⎤⎛ ⎞∴ = − − = −⎜ ⎟⎢ ⎥

⎝ ⎠⎣ ⎦ 

Consider upward deflection of cantilever beam at  A due to concentrated load  R A.

[Appendix C, Cantilever beam with concentrated load at tip.]

 Relevant equation from Appendix C:3 3

3 3

 A A

 PL R Lv

 EI EI = =  

Compatibility equation for deflection at  A:

3 37 70

12 3 4

 A A

 PL R L P  R

 EI EI − + = ∴ = ↑   Ans. 

Equilibrium equations for entire beam: 

0

7 3 34 4 4

 y A B

 B

 F R R P 

 P P P  R P 

Σ = + − =

∴ = − = − = ↓   Ans.

 3

02

 B B A

 L M M R L P 

⎛ ⎞Σ = − + =⎜ ⎟

⎝ ⎠ 

3 7 3( ) (ccw)

2 4 2 4 4 B A

 L P PL PL PL M R L P L

⎛ ⎞∴ = − = − = =⎜ ⎟

⎝ ⎠  Ans.

 

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11.25 For the beam and loading shown below,derive an expression for the reactions at

supports  A  and  B. Assume that  EI is constant

for the beam.

Fig. P11.25

Solution

Choose the reaction force at A as the redundant; therefore, the released beam is a cantilever.

Consider downward deflection of cantilever beam at  A due to uniformly distributed load.

[Appendix C, Cantilever beam with uniformly distributed load.]

 Relevant equation from Appendix C:2

2 2(6 4 )24

 A

wxv L Lx x

 EI = − − +   (elastic curve) 

22 42

3Let ,

2

( ) 3 3 176 4 ( ) ( )

24 2 2 48 A

 L x L L

w L L L wLv L L

 EI EI 

= =

⎡ ⎤⎛ ⎞ ⎛ ⎞∴ = − − + = −⎢ ⎥⎜ ⎟ ⎜ ⎟

⎝ ⎠ ⎝ ⎠⎢ ⎥⎣ ⎦ 

Consider upward deflection of cantilever beam at  A due to concentrated load  R A.

[Appendix C, Cantilever beam with concentrated load at tip.]

 Relevant equation from Appendix C:3 3

3 3

 A A

 PL R Lv

 EI EI = =  

Compatibility equation for deflection at  A:4 317 17

048 3 16

 A A

wL R L wL R

 EI EI − + = ∴ = ↑   Ans. 

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Equilibrium equations for entire beam:

3 3 17 7 702 2 16 16 16

 y A B B

wL wL wL wL wL F R R RΣ = + − = ∴ = − = = ↑   Ans.

3 30

2 4 B B A

wL L M M R L

  ⎛ ⎞⎛ ⎞Σ = − + =⎜ ⎟⎜ ⎟

⎝ ⎠⎝ ⎠ 

2 2 2 29 17 9( ) (cw)

8 16 8 16 16 B A

wL wL wL wL wL M R L L∴ = − = − = − =   Ans.