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fisica1-youn-e-freedman-exercicios-resolvidos

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2<br />

1<br />

9.56: a) Ι =<br />

1 Μa b) Ι = Μb<br />

12<br />

12<br />

2<br />

=<br />

M<br />

. . , Ιcm<br />

L and d L h ,<br />

12<br />

2<br />

9.57: In Eq ( 919) ( 2 ) so<br />

2<br />

⎡ 1 L ⎤<br />

2 ⎛ ⎞<br />

Ιp = Μ ⎢ L + ⎜ − h⎟<br />

⎥<br />

⎢⎣<br />

12 ⎝ 2 ⎠ ⎥⎦<br />

⎡ 1 2 1 2<br />

= Μ<br />

⎢<br />

L + L − Lh + h<br />

⎣12<br />

4<br />

⎡1<br />

2<br />

2⎤<br />

= Μ<br />

⎢<br />

L − Lh + h<br />

⎥<br />

,<br />

⎣3<br />

⎦<br />

which is the same as found in Example 9.12.<br />

=<br />

−<br />

⎤<br />

⎥<br />

⎦<br />

2<br />

9.58: The analysis is identical to that of Example 9.13, with the lower limit in the integral<br />

2<br />

being zero and the upper limit being R, and the mass Μ = πLρR . The result is<br />

2<br />

Ι = 1<br />

ΜR , as given in Table ( 9 .2(f)).<br />

2<br />

9.59: With dm = dx<br />

L<br />

M<br />

L<br />

3<br />

2 M M x M<br />

Ι = ∫ x dx = =<br />

L L 3 3<br />

0<br />

L<br />

0<br />

2<br />

L .

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