29.06.2016 Views

Thomas Calculus 13th [Solutions]

  • No tags were found...

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Section 13.2 Integrals of Vector Functions; Projectile Motion 939<br />

2<br />

(17.80)<br />

32<br />

R sin128 7.80ft the engine traveled about 7.80ft in1sec the engine velocity was<br />

about 7.80 ft/sec<br />

36. (a) r( t) ( x( t)) i ( y( t)) j ; where x( t) (145cos 23 14) t and<br />

(b)<br />

2<br />

y( t) 2.5 (145sin 23 ) t 16 t .<br />

2 2<br />

( v0<br />

sin ) (145sin 23 )<br />

v0 y which is reached at t<br />

sin 145sin 23<br />

max 2g<br />

64<br />

1.771seconds.<br />

(c) For the time, solve<br />

145sin 23 145sin 23 160<br />

32<br />

2.5 2.5 52.655feet,<br />

2<br />

y 2.5 (145sin 23 ) t 16t 0for t , using the quadratic formula<br />

2<br />

t 3.585sec. Then the range at t 3.585 is about<br />

x<br />

(145cos 23 14)(3.585) 428.311 feet.<br />

(d) For the time, solve<br />

145sin 23 145sin 23 1120<br />

32<br />

2<br />

y 2.5 (145sin 23 ) t 16t 20 for t, using the quadratic formula<br />

2<br />

t 0.342 and 3.199seconds. At those times the ball is about<br />

x (0.342) (145cos 23 14)(0.342) 40.860feet from home plate and<br />

x (3.199) (145cos 23 14)(3.199) 382.195feet from home plate.<br />

(e) Yes. According to part (d), the ball is still 20 feet above the ground when it is 382 feet from home plate.<br />

g<br />

32<br />

37.<br />

2<br />

d r<br />

dt<br />

d r<br />

dt<br />

P( t) dt kt dr<br />

1<br />

dt v( t)<br />

k gj P( t)<br />

k and Q( t ) g j P ( t ) dt kt v ( t ) e e v ( t ) Q( t ) dt<br />

2<br />

ge kt e kt dt ge kt<br />

kt<br />

e<br />

g kt<br />

1 ,<br />

k<br />

k<br />

e<br />

j j C j C where C g C 1 ; apply the initial condition:<br />

dr<br />

g g<br />

t 0 v0 v<br />

dt 0 v<br />

k 0 v<br />

k 0<br />

( cos ) i ( sin ) j j C C ( cos ) i sin j<br />

dr<br />

kt<br />

g kt g<br />

v<br />

dt 0e e v<br />

k k 0<br />

cos i sin j,<br />

r v 0 e cos i e v 0 sin j dt<br />

v kt<br />

0 kt<br />

gt g<br />

e<br />

e<br />

k k k k<br />

cos i sin j C ; apply the initial condition:<br />

v0 2<br />

v0 g v0 sin<br />

v0 g v0<br />

sin<br />

k 2 k 2 2 k 2<br />

k<br />

k k<br />

r(0) 0 cos i j C C cos i j<br />

v kt v kt g<br />

kt<br />

t e e kt e<br />

k k k<br />

r i j<br />

0 0<br />

( ) 1 cos 1 sin 1<br />

2<br />

kt<br />

g<br />

k<br />

kt<br />

g<br />

k<br />

38. (a) r( t) x( t) i y( t) j ; where<br />

152 0.12t<br />

x( t) 1 e (cos 20 ) and<br />

0.12<br />

y( t) 3<br />

152 0.12t<br />

32<br />

0.12t<br />

1 e (sin 20 ) 1 0.12t e<br />

0.12 2<br />

0.12<br />

(b) Solve graphically using a calculator or CAS: At t 1.484 seconds the ball reaches a maximum height of<br />

about 40.435feet.<br />

(c) Use a graphing calculator or CAS to find that y 0 when the ball has traveled for 3.126 seconds. The<br />

range is about<br />

152<br />

0.12<br />

0.12(3.126)<br />

x(3.126) 1 e (cos 20 ) 372.311 feet.<br />

(d) Use a graphing calculator or CAS to find that y 30 for t 0.689 and 2.305 seconds, at which times<br />

the ball is about x (0.689) 94.454feet and x (2.305) 287.621feet from home plate.<br />

(e) Yes, the batter has hit a home run since a graph of the trajectory shows that the ball is more than 14 feet<br />

above the ground when it passes over the fence.<br />

Copyright<br />

2014 Pearson Education, Inc.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!