Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 8 - Rotational Motion - Problems - Page 226: 69

Answer

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Work Step by Step

a. There is no net external torque on the wheel-people system, so its net angular momentum is conserved. We assume the people have no initial angular momentum. The final angular velocity is the same for everything. $$L_{i}=L_{f}$$ $$I_i \omega_i = I_f \omega_f$$ $$\omega_f =\omega_i \frac{I_i }{I_f} $$ Find initial and final moments of inertia. $$I_i=1360 kg \cdot m^2$$ $$I_f=1360 kg \cdot m^2 + 4M_{person}R_{wheel}^2=2506.6 kg \cdot m^2$$ The initial frequency is given, so evaluate to find the final frequency. $$\omega_f =(0.80rad/s) \frac{I_i }{I_f}=0.43 rad/s $$ b. The people jump off the merry-go-round radially. They exert no torque on the merry-go-round and do not change the angular momentum of the merry-go-round, which would therefore keep its initial angular velocity of 0.80 rad/s.
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