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10.76: (a) 1 2 1<br />

mgh = mv + Iω<br />

2 (1)<br />

2 2<br />

2 ⎛ 1 2 ⎞<br />

I = I<br />

rim<br />

+ I<br />

spokes<br />

= M<br />

rR<br />

+ 6⎜<br />

msR<br />

⎟<br />

⎝ 3 ⎠<br />

Uniform density means: m = λ πR and m = λR.<br />

No slipping means that ω = v R.<br />

r<br />

2<br />

s<br />

r<br />

+ ms<br />

= 2πRλ<br />

+ 6Rλ<br />

= 2Rλ<br />

+<br />

Also, = m<br />

( π 3)<br />

m substituting into (1) gives<br />

2Rλ<br />

1<br />

2<br />

( π + 3) gh = ( 2Rλ)( π + 3)( Rω)<br />

ω =<br />

( π + 3)<br />

gh<br />

2<br />

R ( π + 2)<br />

=<br />

and v = Rω = 26.0 m s<br />

2<br />

1 ⎡<br />

+ 2<br />

2<br />

⎢ πRλR<br />

⎣<br />

⎛ 1<br />

+ 6⎜<br />

πRR<br />

⎝ 3<br />

2<br />

( π + 3)( 9.80 m s )( 58.0 m)<br />

2<br />

( 0.210 m) ( π + 2)<br />

2<br />

2<br />

⎞⎤<br />

⎟⎥ω<br />

⎠⎦<br />

2<br />

= 124 rad<br />

s<br />

(b) Doubling the density would have no effect because it does not appear in the answer.<br />

1<br />

ω α ,<br />

R<br />

so doubling the diameter would double the radius which would reduce<br />

ω by half, but v = Rω would be unchanged.<br />

10.77: a) The front wheel is turning at ω = 1.00 rev s = 2π<br />

rad s.<br />

υ = rω = ( 0.330 m)(2π<br />

rad s) = 2.07 s<br />

b) ω = v r = ( 2.07 m s) (0.655 m = 3.16 rad s = 0.503 rev s<br />

c) ω = v r = ( 2.07 m s) (0.220 m) = 9.41rad s = 1.50 rev s<br />

10.78: a) The kinetic energy of the ball when it leaves the tract (when it is still rolling<br />

2<br />

without slipping) is (7 10)<br />

mv and this must be the work done by gravity, W = mgh, so<br />

v = 10gh 7. The ball is in the air for a time t = 2y<br />

g,<br />

so x = vt = 20hy<br />

7.<br />

b) The answer does not depend on g, so the result should be the same on the moon.<br />

c) The presence of rolling friction would decrease the distance.<br />

2<br />

d) For the dollar coin, modeled as a uniform disc, K = (3 4) mv , and so x = 8hy<br />

3.

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