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Thomas Calculus 13th [Solutions]

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936 Chapter 13 Vector-Valued Functions and Motion in Space<br />

23. (a)<br />

(b)<br />

2 2<br />

v0 v0<br />

2<br />

2 2 2<br />

R v<br />

g<br />

0 v0<br />

9.8m/s<br />

sin 2 10m = (sin 90 ) 98 m /s 9.9 m/s;<br />

2<br />

(9.9 m/s )<br />

6m (sin 2 ) sin 2 0.59999 2 36.87 or 143.12 18.4 or 71.6<br />

2<br />

9.8m/s<br />

24.<br />

v 0<br />

6<br />

5 10 m/s and x 40cm 0.4 m; thus x ( v0<br />

cos ) t 0.4 m<br />

6<br />

(5 10 m/s)(cos0 ) t<br />

t<br />

6 8<br />

2<br />

0.08 10 s 8 10 s; also, y y 1<br />

0 ( v0 sin ) t gt<br />

2<br />

y<br />

6 8 1 2 8 2 14<br />

12<br />

(5 10 m/s)(sin 0 )(8 10 s) (9.8m/s )(8 10 s) 3.136 10 m or 3.136 10 cm.<br />

2<br />

12<br />

Therefore, it drops 3.136 10 cm.<br />

25.<br />

2 2<br />

0<br />

(400m/s)<br />

2<br />

v<br />

g<br />

R sin 2 16,000 m sin 2 sin 2 0.98 2 78.5 or 2 101.5 39.3<br />

or 50.7<br />

9.8m/s<br />

26. (a)<br />

2 2 2<br />

0 0 0<br />

(2 v ) 4v v<br />

g g g<br />

R sin 2 sin 2 4 sin or 4 times the original range.<br />

(b) Now, let the initial range be<br />

2 2<br />

0 v0<br />

( pv ) 2<br />

g<br />

g<br />

2<br />

v<br />

R 0<br />

sin 2 . Then we want the factor p so that pv<br />

g<br />

0 will double the range<br />

sin 2 2 sin 2 p 2 p 2 or about 141%. The same percentage will<br />

approximately double the height:<br />

2 2<br />

0 v0<br />

( pv sin ) 2( sin ) 2<br />

p<br />

2g<br />

2g<br />

2 p 2.<br />

27. The projectile reaches its maximum height when its vertical component of velocity is zero<br />

2<br />

dy<br />

v v 1 v v v<br />

v0 sin gt 0 t ymax ( v0 sin )<br />

g<br />

dt g g 2 g g 2g<br />

2<br />

( v0<br />

sin )<br />

2g<br />

2 2<br />

0 sin 0 sin 0 sin ( 0 sin ) ( 0 sin )<br />

1<br />

0 2<br />

. To find the flight time we find the time when the projectile lands: ( v sin ) t gt 0<br />

1<br />

0 2<br />

2v<br />

sin<br />

g<br />

0<br />

t v sin gt 0 t 0 or t . Since t 0 is the time when the projectile is fired, then<br />

2v<br />

sin<br />

g<br />

0<br />

t is the time when the projectile strikes the ground. The range is the value of the horizontal<br />

2 2<br />

2v sin 2v sin v v<br />

g 0<br />

g g g<br />

0 0 0 0<br />

component when t R x ( v cos ) (2sin cos ) sin 2 . The range is<br />

largest when 2 1 45 .<br />

28. When marble A is located R units downrange, we have<br />

time the height of marble A is<br />

R<br />

0 0 v cos<br />

x ( v cos ) t R ( v cos ) t t . At that<br />

1 2<br />

y y 1<br />

0 ( v0 sin ) t gt ( v<br />

2 0 sin )<br />

R g R<br />

v cos 2 v cos<br />

0 0<br />

2<br />

2<br />

0<br />

2<br />

1 R<br />

2 v cos<br />

y R tan g . The height of marble B at the same time<br />

2 2<br />

0<br />

R<br />

v0 cos<br />

t seconds is<br />

1 2<br />

1 R<br />

2 2 v cos<br />

2<br />

h R tan gt R tan g . Since the heights are the same, the marbles collide regardless of<br />

the initial velocity v 0 .<br />

2 2<br />

0<br />

Copyright<br />

2014 Pearson Education, Inc.

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