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10.32:<br />

I<br />

= mL<br />

1 2 1<br />

2<br />

2<br />

= ( 117 kg)(2.08 m) = 42.2 kg ⋅ m<br />

2 2<br />

τ 1950 N ⋅ m<br />

2<br />

a) α = =<br />

46.2 rad/s .<br />

2<br />

42.2 kg ⋅ m<br />

=<br />

I<br />

2<br />

b) ω = 2αθ<br />

= 2(46.2 rad/s )(5.0 rev×<br />

2π<br />

rev) = 53.9 rad/s.<br />

1 2<br />

c) From either W = K = ω or Eq. (10.24),<br />

2<br />

4<br />

W = τθ = (1950 N.m)(5.00 rev×<br />

2π<br />

rad/rev) = 6.13×<br />

10 J.<br />

d), e) The time may be found from the angular acceleration and the total angle, but the<br />

instantaneous power is also found from P = τω = 105 kW(141hp).<br />

The average power is<br />

half of this, or 52 .6 kW.<br />

3 ⎛<br />

⎛ π rad/s ⎞⎞<br />

10.33: a) τ = P / ω = (150×<br />

10 W) ⎜(400 rev/min) ⎜ ⎟⎟<br />

= 358 N ⋅ m.<br />

⎝<br />

⎝ 30 rev/min ⎠⎠<br />

3<br />

b) If the tension in the rope is F , F = w and so w = τ/<br />

R = 1.79×<br />

10 N.<br />

c) Assuming ideal efficiency, the rate at which the weight gains potential energy is the<br />

power output of the motor, or wv = P, so v = P w = 83.8 m/s. Equivalently, v = ωR.<br />

10.34: As a point, the woman’s moment of inertia with respect to the disk axis is<br />

and so the total angular momentum is<br />

⎛ 1 ⎞ 2<br />

L = Ldisk<br />

+ Lwoman<br />

= ( Idisk<br />

+ Iwoman)<br />

ω = ⎜ M + m⎟R<br />

ω<br />

⎝ 2 ⎠<br />

⎛ 1<br />

⎞<br />

2<br />

= ⎜ 110 kg + 50.0 kg⎟(4.00 m) (0.500 rev/s×<br />

2π<br />

rad/rev)<br />

⎝ 2<br />

⎠<br />

= 5.28×<br />

10<br />

3<br />

kg ⋅ m<br />

2<br />

/s.<br />

2<br />

mR ,<br />

2<br />

10.35: a) mvr sinφ = 115 kg ⋅ m /s,<br />

with a direction from the right hand rule of into the<br />

page.<br />

2<br />

b) dL dt = τ = ( 2 kg)( 9.8 N kg) ⋅ ( 8 m) ⋅ sin( 90° − 36.9°<br />

) = 125 N ⋅ m = 125 kg ⋅ m s ,<br />

out of the page.<br />

2

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