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Thomas Calculus 13th [Solutions]

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472 Chapter 6 Applications of Definite Integrals<br />

15. The slab is a disk of area<br />

work to pump the oil in this slab, W , is 57<br />

2<br />

2 y<br />

x , thickness y , and height below the top of the tank (10 y ). So the<br />

2<br />

3 4 10<br />

y<br />

2<br />

(10 y ) . The work to pump all the oil to top of the tank is<br />

2<br />

10<br />

57 2 3 57 10y<br />

y<br />

W 10 y y dy<br />

11,875 ft lb 37,306 ft-lb<br />

0 4 4 3 4<br />

0<br />

y<br />

2<br />

16. Each slab of oil is to be pumped to a height of 14 ft. So the work to pump a slab is (14 y )( ) and since<br />

2<br />

2 2 3<br />

the tank is half full and the volume of the original cone is V 1 r h 1 5 (10) 250 ft , half the<br />

3 3 3<br />

volume<br />

250<br />

6<br />

3<br />

ft , and with half the volume the cone is filled to a height y, 250 1 y<br />

y<br />

6 3 4<br />

3<br />

3 3 4 500<br />

500 2 3<br />

14<br />

So<br />

57 57 y y<br />

W 14 y y dy<br />

60,042 ft-lb.<br />

0 4 4 3 4<br />

0<br />

17. The typical slab between the planes at y and y y has a volume of<br />

V<br />

2<br />

y<br />

2<br />

(radius) (thickness)<br />

20<br />

2<br />

3<br />

y 100 y ft . The force F required to lift the slab is equal to its weight:<br />

2<br />

F 51.2 V 51.2 100 y lb F 5120 y lb The distance through which F must act is about<br />

3<br />

500 ft.<br />

30 30<br />

(30 y ) ft. The work it takes to lift all the kerosene is approximately W W 5120 (30 y) y ft-lb<br />

0 0<br />

which is a Riemann sum. The work to pump the tank dry is the limit of these sums:<br />

30<br />

2 30<br />

900<br />

0<br />

5120 (30 ) 5120 30 y<br />

W y dy y<br />

2 5120 2<br />

(5120)(450 ) 7,238,229.48 ft-lb<br />

0<br />

18. (a) Follow all the steps of Example 5 but make the substitution of 64.5 lb for 57 lb . Then,<br />

3<br />

3<br />

ft ft<br />

8<br />

8<br />

64.5 2 64.5 10 y y 64.5 10 8 8 64.5 3<br />

W (10 y) y dy<br />

8 10 2 64.5 8<br />

0 4 4 3 4 4 3 4 4 3 3<br />

0<br />

3<br />

21.5 8 34,582.65 ft-lb<br />

3 4 3 4 3<br />

(b) Exactly as done in Example 5 but change the distance through which F acts to distance (13 y ) ft.<br />

3 4 8<br />

8 2 13<br />

3 4<br />

3<br />

3<br />

Then 57 57 y y<br />

W (13 y) y dy<br />

57 13 8 8 57 8 13 2 57 8 7<br />

0 4 4 3 4 4 3 4 4 3 3 4<br />

0<br />

2<br />

(19 )(8 )(7)(2) 53,482.5 ft-lb<br />

19. The typical slab between the planes at y and y y has a volume of about<br />

2<br />

3<br />

y y ft . The force F( y ) required to lift this slab is equal to its weight: F ( y) 73<br />

V<br />

2<br />

(radius) (thickness)<br />

2<br />

73 y y 73 y y lb. The distance through which F( y ) must act to lift the slab to the top of the<br />

reservoir is about (4 y ) ft, so the work done is approximately W 73 y(4 y) y ft-lb. The work done<br />

n<br />

lifting all the slabs from y 0 ft to y 4 ft is approximately W 73 yk<br />

4 yk<br />

y ft-lb. Taking the limit<br />

k 0<br />

V<br />

Copyright<br />

2014 Pearson Education, Inc.

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