University Physics with Modern Physics (14th Edition)

Published by Pearson
ISBN 10: 0321973615
ISBN 13: 978-0-32197-361-0

Chapter 10 - Dynamics of Rotational Motion - Problems - Exercises - Page 332: 10.50

Answer

(a) $\omega = 1.71~rad/s$ (b) During the collision, the pivot exerts an external force, which causes the linear momentum to change. However, the force from the pivot exerts zero torque. Therefore, angular momentum is conserved.

Work Step by Step

(a) We can use conservation of angular momentum to solve this question. Let $v_1$ be the initial speed of the raven and let $v_2$ be the speed of the raven after it rebounds. $L_2=L_1$ $I\omega-mv_2r = mv_1r$ $\frac{1}{3}ML^2\omega = mr(v_1+v_2)$ $\omega = \frac{3mr(v_1+v_2)}{ML^2}$ $\omega = \frac{(3)(1.1~kg)(0.75~m)(5.0~m/s+2.0~m/s)}{(4.5~kg)(1.5~m)^2}$ $\omega = 1.71~rad/s$ (b) During the collision, the pivot exerts an external force, which causes the linear momentum to change. However, the force from the pivot exerts zero torque. Therefore, angular momentum is conserved.
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