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J<br />

10.98: The velocity of the center of mass will change by ∆ v = , and the angular<br />

velocity will change by ∆ω<br />

=<br />

J x x<br />

I<br />

( − cm )<br />

⋅The change is velocity of the end of the bat will<br />

J J ( x − xcm)<br />

xcm<br />

then be ∆vend<br />

= ∆vcm<br />

_ ∆ωxcm<br />

= −<br />

⋅ Setting<br />

m Ι<br />

∆ v<br />

end<br />

= 0 allows cancellation of J,<br />

and gives Ι = ( x − xcm)<br />

xcmm,<br />

which when solved for x<br />

is<br />

−2<br />

2<br />

Ι (5.30×<br />

10 kg ⋅ m )<br />

x = + xcm<br />

=<br />

+ (0.600 m) = 0.710 m.<br />

x m (0.600 m)(0.800 kg)<br />

cm<br />

cm<br />

m<br />

10.99: In Fig. (10.34(a)), if the vector<br />

r , and hence the vector L are not horizontal but make an angle β with the horizontal, the<br />

torque will still be horizontal (the torque must be perpendicular to the vertical weight).<br />

The magnitude of the torque will be ω r cos β , and this torque will change the direction<br />

of the horizontal component of the angular momentum, which has magnitude L cos β .<br />

Thus, the situation of Fig. (10.36) is reproduced, but with L<br />

expression found in Eq. (10.36) becomes<br />

horiz<br />

instead of L . Then, the<br />

dφ<br />

Ω = =<br />

dt<br />

d L<br />

dt<br />

L<br />

horiz<br />

=<br />

L<br />

τ<br />

horiz<br />

mgr cos β<br />

=<br />

Lcos<br />

β<br />

ωr<br />

= ⋅<br />

Ιω

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