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10.95: a) The initial angular momentum with respect to the pivot is mvr,<br />

and the<br />

2<br />

final total moment of inertia is I + mr , so the final angular velocity is<br />

2<br />

ω = mvr ( mr + I ).<br />

b) The kinetic energy after the collision is<br />

1 2 2<br />

K = ω ( mr + I ) = ( M + m)<br />

gh,<br />

or<br />

2<br />

ω =<br />

2<br />

( M + )<br />

m gh<br />

.<br />

2<br />

( mr + I )<br />

2<br />

⎛ m ⎞<br />

c) Substitution of Ι = Μr into either of the result of part (a) gives ω = ⎜ ⎟( v r),<br />

⎝ m + M ⎠<br />

and into the result of part (b), ω = 2gh(1<br />

r),<br />

which are consistent with the forms for v.<br />

10.96: The initial angular momentum is Ιω1 − mRv1<br />

, with the minus sign indicating that<br />

runner’s motion is opposite the motion of the part of the turntable under his feet. The<br />

2<br />

final angular momentum is ω<br />

2<br />

( Ι + mR ), so<br />

Ιω1<br />

− mRv1<br />

ω2<br />

=<br />

2<br />

Ι + mR<br />

2<br />

(80 kg ⋅ m )(0.200 rad s) − (55.0 kg)(3.00 m)(2.8 m s)<br />

=<br />

2<br />

2<br />

(80 kg ⋅ m ) + (55.0 kg)(3.00 m)<br />

= −0.776 rad s,<br />

where the minus sign indicates that the turntable has reversed its direction of motion (i.e.,<br />

the man had the larger magnitude of angular momentum initially).<br />

10.97: From Eq. (10.36),<br />

ωr<br />

Ω =<br />

Ι ω<br />

2<br />

(50.0 kg)(9.80 m s )(0.040 m)<br />

=<br />

= 12.7 rad<br />

2<br />

(0.085 kg ⋅ m )((6.0m s) (0.33 m))<br />

s,<br />

or 13<br />

rad<br />

s to two figures, which is quite large.

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