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10.43: a) From conservation of angular momentum,<br />

2<br />

I1<br />

( 1 2)<br />

MR<br />

ω2<br />

= ω1<br />

= ω<br />

2 1<br />

2<br />

I + mR 1 2 MR + mR<br />

0<br />

( 70)<br />

( )<br />

3.0 rad s<br />

=<br />

= 1.385 rad s<br />

1+<br />

2 120<br />

2<br />

1<br />

= ω1<br />

1+<br />

2m<br />

M<br />

or 1.39<br />

rad s to three figures<br />

2<br />

2<br />

1<br />

=<br />

=<br />

2<br />

= (<br />

0<br />

) ω2<br />

= J.<br />

K and<br />

b) ( 1 2)( 1 2)( 120 kg)( 2.00 m) ( 3.00 rad s) 1.80 kJ,<br />

2 2<br />

( 1 2) I + ( 70 kg)( 2.00 m)<br />

499<br />

K In changing the parachutist’s horizontal<br />

component of velocity and slowing down the turntable, friction does negative work.<br />

10.44: Let the width of the door be l;<br />

ω =<br />

=<br />

mv( l 2)<br />

=<br />

2<br />

2<br />

( 1 3) Ml + m( l 2)<br />

( 0.500 kg)( 12.0 m s)( 0.500 m)<br />

2<br />

( 1 3)( 40.0 kg)( 1.00 m) + ( 0.500 kg)( 0.500 m)<br />

L<br />

I<br />

2<br />

= 0.223 rad<br />

s.<br />

Ignoring the mass of the mud in the denominator of the above expression gives<br />

ω = 0.225 rad s, so the mass of the mud in the moment of inertia does affect the third<br />

significant figure.<br />

10.45: Apply conservation of angular momentum L r , with the axis at the nail. Let object<br />

A be the bug and object B be the bar.<br />

Initially, all objects are at rest and L = 0 1<br />

.<br />

Just after the bug jumps, it has angular momentum in one direction of rotation and the<br />

bar is rotating with angular velocity ω in the opposite direction.<br />

L<br />

2<br />

1<br />

= m<br />

L = L<br />

2<br />

3mAv<br />

ωB<br />

=<br />

m r<br />

v r − I ω<br />

A A<br />

gives m v<br />

B<br />

A<br />

B<br />

A<br />

B<br />

A<br />

B<br />

where r = 1.00 m and I<br />

r =<br />

1<br />

3<br />

m<br />

B<br />

= 0.120 rad s<br />

r<br />

2<br />

ω<br />

B<br />

B<br />

=<br />

1<br />

3<br />

m<br />

B<br />

r<br />

2

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