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9.40: a) In the expression of Eq. (9.16), each term will have the mass multiplied by<br />

3<br />

f and the distance multiplied by f , and so the moment of inertia is multiplied by<br />

3 2 5<br />

5<br />

8<br />

f ( f ) = f . b) (2.5)(48) = 6.37 × 10 .<br />

9.41: Each of the eight spokes may be treated as a slender rod about an axis through an<br />

end, so the moment of inertia of the combination is<br />

2 ⎛ mspoke<br />

⎞ 2<br />

I = mrimR<br />

+ 8 ⎜ ⎟ R<br />

⎝ 3 ⎠<br />

⎡ 8 ⎤<br />

2<br />

=<br />

⎢<br />

(1.40 kg) + (0.20 kg) (0.300 m)<br />

⎣ 3 ⎥<br />

⎦<br />

= 0.193 kg ⋅ m<br />

2<br />

9.42: a) From Eq. (9.17), with I from Table (9.2(a)),<br />

1 2 1<br />

2 rev 2π<br />

rad rev<br />

K = mL ω = (117 kg)(2.08 m) (2400 × )<br />

2 12 24<br />

min 60 s min<br />

b) From mgy = K,<br />

1 2 2<br />

6<br />

y<br />

K<br />

= mg<br />

6<br />

( 1 .3×<br />

10 J) 3<br />

= 1.16 × 10 m = 1.16 km.<br />

=<br />

(117 kg)(9.80 m s<br />

2<br />

)<br />

= 1.3×<br />

10<br />

J.<br />

2<br />

9.43: a) The units of moment of inertia are [kg][m ]<br />

and the units of ω are equivalent<br />

−1<br />

2<br />

to [s ] and so the product 1 Iω has units equivalent to −2<br />

2<br />

]<br />

2<br />

[kg ⋅ m ⋅ s ] = [kg ⋅ (m s) ,<br />

which are the units of Joules. A radian is a ratio of distances and is therefore unitless.<br />

b) K = π<br />

2 Iω 2 1800 , when is in rev min.<br />

9.44: Solving Eq. (9.17) for I,<br />

2K<br />

2(0.025J)<br />

−3<br />

2<br />

I = =<br />

= 2.25×<br />

10 kg ⋅ m .<br />

2 2π<br />

rad s 2<br />

ω (45 rev min × )<br />

60 rev min

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