p08 096

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96. (Third problem in Cluster 1)

(a) When there is no change in potential energy, Eq. 8-24 leads to

W

app

= ∆K =

1

2

m



v

2

− v

2

0



.

Therefore, ∆E = 6.0

× 10

3

J.

(b) From the above manipulation, we see W

app

= 6.0

× 10

3

J. Also, from Chapter 2, we know that

t = ∆v/a =10 s. Thus, using Eq. 7-42,

P

avg

=

W

t

=

6.0

× 10

3

10

=600 W .

(c) and (d) The constant applied force is ma =30 N and clearly in the direction of motion, so Eq. 7-48

provides the results for instantaneous power

P =

F

· v =



300 W

for v =10 m/s

900 W

for v =30 m/s

We note that the average of these two values agrees with the result in part (b).


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