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6.5: a) See Exercise 5.37. The needed force is<br />

F<br />

2<br />

µ<br />

kmg<br />

(0.25)(30 kg)(9.80 m / s )<br />

=<br />

=<br />

cos φ − µ sinφ<br />

cos30° − (0.25)sin 30°<br />

k<br />

= 99.2 N,<br />

keeping extra figures. b) Fs cos φ = (99.2 N)(4.50 m) cos 30°<br />

= 386.5 J , again keeping an<br />

extra figure. c) The normal force is mg + F sinφ<br />

, and so the work done by friction is<br />

2<br />

− (4.50 m)(0.25)((30 kg)(9.80 m / s ) + (99.2 N)sin 30°<br />

) = −386.5 J . d) Both the normal<br />

force and gravity act perpendicular to the direction of motion, so neither force does work.<br />

e) The net work done is zero.<br />

6.6: From Eq. (6.2),<br />

Fs cosφ = (180 N)(300 m)cos15.0°<br />

= 5.22 × 10<br />

4<br />

J.<br />

6<br />

6.7: 2Fs cosφ<br />

= 2(1.80×<br />

10<br />

3<br />

9<br />

N)(0.75×<br />

10 m)cos14°<br />

= 2.62 × 10 J,<br />

9<br />

or 2.6 × 10 J to<br />

two places.<br />

6.8: The work you do is:<br />

r<br />

F ⋅ s<br />

r = (( 30N)ˆ i − (40N) ˆ) j ⋅ (( −9.0m)ˆ<br />

i − (3.0m) ˆ) j<br />

= ( 30 N)( −9.0 m) + ( −40 N)( −3.0 m)<br />

= −270 N ⋅ m + 120 N ⋅ m = −150 J<br />

6.9: a) (i) Tension force is always perpendicular to the displacement and does no work.<br />

(ii) Work done by gravity is − mg ( y 2<br />

− y1).<br />

When y<br />

1<br />

= y2<br />

, W<br />

mg<br />

= 0 .<br />

b) (i) Tension does no work.<br />

(ii) Let l be the length of the string. = −mg<br />

( y − y ) 1<br />

= −mg(2l)<br />

= 25.1J<br />

W mg<br />

2<br />

−<br />

The displacement is upward and the gravity force is downward, so it does negative<br />

work.

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