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9.90: a) In the case that no energy is lost, the rebound height h′ is related to the speed<br />

2<br />

υ<br />

v by h ′<br />

h<br />

= , and with the form for h given in Example 9.9, ′ = . b) Considering<br />

2g<br />

h<br />

1+<br />

M 2m<br />

the system as a whole, some of the initial potential energy of the mass went into the<br />

kinetic energy of the cylinder. Considering the mass alone, the tension in the string did<br />

work on the mass, so its total energy is not conserved.<br />

9.91: We can use Κ ( cylinder) = 250 J to find ω for the cylinder and v for the mass.<br />

Ι<br />

= MR<br />

1 2 1<br />

2<br />

2<br />

= ( 10.0 kg)(0.150 m) = 0.1125 kg ⋅ m<br />

2<br />

2<br />

2<br />

K = 1 Iω<br />

so ω = 2K<br />

I =<br />

2<br />

66.67 rad s<br />

v = Rω<br />

=10.0 m s<br />

Use conservation of energy K<br />

1<br />

+ U1<br />

= K<br />

2<br />

+ U<br />

2.<br />

Take y = 0 at lowest point of the<br />

mass, so y = and y = , the distance the mass descends. K = U = so U = .<br />

2<br />

0<br />

1<br />

h<br />

1 2 1 2<br />

=<br />

2<br />

mv +<br />

2<br />

I , where m =<br />

2<br />

MR and<br />

2<br />

1 2 1 2<br />

= mv Mv<br />

2<br />

4<br />

mgh ω<br />

12.0 kg<br />

1 2 1 2<br />

For the cylinder, I = 1 ω = v R,<br />

so Iω<br />

= Mv .<br />

mgh +<br />

2<br />

v ⎛ M ⎞<br />

h = ⎜1<br />

+ ⎟ = 7.23 m<br />

2g<br />

⎝ 2 m ⎠<br />

2<br />

4<br />

1 2<br />

0<br />

1<br />

K2

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