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8.78: The speed of the block after the bullet has passed through (but before the block has<br />

begun to rise; this assumes a large force applied over a short time, a situation<br />

characteristic of bullets) is<br />

V<br />

=<br />

2gy<br />

=<br />

2<br />

2(9.80 m/s )(0.45×<br />

10<br />

−2<br />

m) = 0.297 m/s.<br />

The final speed v of the bullet is then<br />

p mv0<br />

− MV M<br />

v = = = v0<br />

− V<br />

m m m<br />

1.00 kg<br />

= 450 m/s −<br />

(0.297 m/s) = 390.6 m/s,<br />

−3<br />

5.00×<br />

10 kg<br />

or 390 m/s to two figures.<br />

8.79: a) Using the notation of Eq. ( 8.24),<br />

K<br />

0<br />

− K<br />

2<br />

1<br />

= mv<br />

2<br />

1<br />

= mv<br />

2<br />

= K<br />

= K<br />

0<br />

0<br />

2<br />

2<br />

1 2<br />

− mvA<br />

2<br />

2<br />

⎛<br />

⎞<br />

⎜ ⎛ m − M ⎞<br />

1−<br />

⎟<br />

⎜ ⎟<br />

⎝ ⎝ m + M ⎠ ⎠<br />

2<br />

⎛ ( m + M ) − ( m − M )<br />

⎜<br />

2<br />

⎝ ( m + M )<br />

⎛ 4mM<br />

⎜<br />

⎝ ( m + M )<br />

b) Of the many ways to do this calculation, the most direct way is to differentiate the<br />

expression of part (a) with respect to M and set equal to zero;<br />

d ⎛ M ⎞<br />

0 = (4mK0)<br />

⎜ ⎟,<br />

or<br />

2<br />

dM ⎝ ( m + M ) ⎠<br />

1 2M<br />

0 = −<br />

2<br />

3<br />

( m + M ) ( m + M )<br />

0 = ( m + M ) − 2M<br />

m = M.<br />

c) From Eq.(8.24), with m<br />

A<br />

= mB<br />

= m, vA<br />

= 0; the neutron has lost all of its kinetic<br />

energy.<br />

2<br />

⎞<br />

⎟ .<br />

⎠<br />

2<br />

⎞<br />

⎟<br />

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