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fisica1-youn-e-freedman-exercicios-resolvidos

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5.28: a) The stopping distance is<br />

2 2<br />

2<br />

v v (28.7 m s)<br />

= =<br />

= 53 m.<br />

2<br />

2a<br />

2µ<br />

kg<br />

2(0.80) (9.80 m s )<br />

b) The stopping distance is inversely proportional to the coefficient of friction and<br />

proportional to the square of the speed, so to stop in the same distance the initial speed<br />

should not exceed<br />

v<br />

µ<br />

µ<br />

k, wet<br />

k,dry<br />

= (28.7 m s)<br />

0.25<br />

0.80<br />

== 16<br />

m s.<br />

5.29: For a given initial speed, the distance traveled is inversely proportional to the<br />

0 .44<br />

coefficient of kinetic friction. From Table 5.1, the ratio of the distances is then = 11.<br />

0.04<br />

5.30: (a) If the block descends at constant speed, the tension in the connecting string<br />

must be equal to the hanging block’s weight, w<br />

B.<br />

Therefore, the friction force µ w k A<br />

on<br />

block A must be equal to w<br />

B,<br />

and w<br />

B<br />

= µ<br />

kwA.<br />

(b) With the cat on board, a = g w − µ 2w<br />

) ( w + 2w<br />

).<br />

(<br />

B k A B A<br />

5.31:<br />

a) For the blocks to have no acceleration, each is subject to zero net force. Considering<br />

the horizontal components,<br />

r<br />

T = f<br />

A,<br />

F = T + fB,<br />

or<br />

r<br />

F = f + f .<br />

Using<br />

f<br />

A<br />

= µ<br />

kgmA<br />

and fB<br />

µ<br />

kgmB<br />

b) T = f A<br />

= µ gm .<br />

k<br />

A<br />

A<br />

B<br />

= gives F r = µ g ( m A<br />

+ m ) .<br />

k<br />

B

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