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Thomas Calculus 13th [Solutions]

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10. Converting to pounds and feet,<br />

2<br />

1/2<br />

0<br />

Chapter 6 Additional and Advanced Exercises 503<br />

2 lb 12 in<br />

2 lb/in 24 lb/ft. Thus,<br />

1 ln 1ft<br />

1 2 1 2<br />

2 2<br />

1/2<br />

F 24x W 24x dx<br />

0<br />

1 1 1<br />

10 32 ft/sec 320<br />

12x 3 ft lb. Since W mv0 mv 1 , where W 3 ft lb, m lb<br />

slugs,<br />

2<br />

1 1<br />

2 320<br />

2 2<br />

and v 1 0 ft/sec, we have 3 v0 v 0 3 640. For the projectile height,<br />

2<br />

s 16t v t (since<br />

s 0 at t 0 )<br />

ds<br />

v0<br />

v 32 t v 0.<br />

At the top of the balls path, v 0 t and the height is<br />

dt<br />

32<br />

2<br />

2<br />

0 0 0<br />

s 16 v v<br />

v v 3 640<br />

32 0<br />

30 ft.<br />

32 64 64<br />

0<br />

n<br />

11. From the symmetry of y 1 x , n even, about the y -axis for 1 x 1, we have x 0. To find y ,<br />

we use the vertical strips technique. The typical strip has center of mass: ( x, y) x ,<br />

1 x<br />

, length: 1 x ,<br />

n<br />

n<br />

width: dx, area: dA 1 x dx , mass: dm 1 dA 1 x dx . The moment of the strip about the x -axis is<br />

n<br />

2<br />

n<br />

2<br />

1 x<br />

1 1 x<br />

1<br />

1 n 2n n<br />

y dm dx M 2 1 2<br />

2x x<br />

1<br />

2 1<br />

2 x dx x x dx x<br />

1 2 0 2 n 1 2n 1<br />

0<br />

n 1 2n<br />

1<br />

( n 1)(2n 1) 2(2n 1) ( n 1) 2 2<br />

2n 3n 1 4n 2 n 1 2n<br />

( n 1)(2n 1) ( n 1)(2n 1) ( n 1)(2n<br />

1) .<br />

n 1 1<br />

Also,<br />

2<br />

1<br />

1 2<br />

0 1 n<br />

x dx 2 x x<br />

1 2 1 n<br />

n<br />

0<br />

n 1 n 1<br />

. Therefore, y<br />

2<br />

n<br />

1 2n<br />

1 1<br />

1 1<br />

1 n<br />

M dA x dx<br />

1 1<br />

M x<br />

M<br />

2<br />

x 2n ( n 1) n<br />

0,<br />

n<br />

M ( n 1)(2n 1) 2n 2n 1 2n<br />

1<br />

is the location of the centroid. As n , y 1<br />

so the limiting position of the centroid is 0,<br />

1<br />

.<br />

2<br />

2<br />

n<br />

M<br />

12. Align the telephone pole along the x -axis as shown<br />

in the accompanying figure. The slope of the top<br />

14.5 9<br />

8 8<br />

length of pole is<br />

1 1<br />

(14.5 9)<br />

40 8 40<br />

5.5 11<br />

8 40 8 80 . Thus, y 9 11 x<br />

8 8 80<br />

1<br />

9<br />

11 x is an equation of the line<br />

8 80<br />

representing the top of the pole. Then<br />

b 2 40 2 40<br />

2<br />

M 1 11 1 11<br />

y x y dx x<br />

0 8 x dx x<br />

80 64 x dx<br />

0 80<br />

a<br />

b 2 40 2 40 2<br />

M y dx 1 11 1 11<br />

0 8 x dx<br />

80 64 x dx<br />

0 80<br />

Thus,<br />

a<br />

calculator to compute the integrals). By symmetry about the x-axis,<br />

0<br />

from the top of the pole.<br />

M y<br />

M<br />

129,700<br />

5623.3<br />

x 23.06 (using a<br />

y so the center of mass is about 23 ft<br />

13. (a) Consider a single vertical strip with center of mass ( x, y ). If the plate lies to the right of the line, then the<br />

moment of this strip about the line x b is ( x b) dm ( x b)<br />

dA the plates first moment about<br />

x b is the integral ( x b) dA x dA b dA M y b A.<br />

(b) If the plate lies to the left of the line, the moment of a vertical strip about the line x b is ( b x)<br />

dm<br />

( b x)<br />

dA the plates first moment about x b is ( b x) dA b dA x dA b A M y .<br />

Copyright<br />

2014 Pearson Education, Inc.

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