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6.1: a) ( 2.40 N) (1.5 m) = 3.60 J b) ( − 0.600 N)(1.50 m) = −0.900<br />

J<br />

c) 3 .60 J − 0.720 J = 2.70 J .<br />

6.2: a) “Pulling slowly” can be taken to mean that the bucket rises at constant speed, so<br />

the tension in the rope may be taken to be the bucket’s weight. In pulling a given length<br />

of rope, from Eq. (6.1),<br />

2<br />

W = Fs = mgs = (6.75 kg) (9.80 m /s )(4.00 m) = 264.6 J.<br />

b) Gravity is directed opposite to the direction of the bucket’s motion, so Eq. (6.2)<br />

gives the negative of the result of part (a), or − 265 J . c) The net work done on the bucket<br />

is zero.<br />

6.3: ( 25.0 N)(12.0 m) = 300 J .<br />

6.4: a) The friction force to be overcome is<br />

or 74 N to two figures.<br />

2<br />

f = µ<br />

k<br />

n = µ<br />

kmg<br />

= (0.25)(30.0 kg)(9.80 m / s ) = 73.5 N,<br />

b) From Eq. (6.1), Fs = ( 73.5 N)(4.5 m) = 331J<br />

. The work is positive, since the worker<br />

is pushing in the same direction as the crate’s motion.<br />

c) Since f and s are oppositely directed, Eq. (6.2) gives<br />

− fs = −( 73.5 N)(4.5 m) = −331J.<br />

d) Both the normal force and gravity act perpendicular to the direction of motion, so<br />

neither force does work. e) The net work done is zero.

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