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 330: 10.20

Answer

(a) $\omega = 33.9~rad/s$ (b) $v = 2.71~m/s$

Work Step by Step

(a) We can set up an equation with the torque from the tension in the string. $\tau = I\alpha$ $TR = (mR^2)(\frac{a}{R})$ $T = ma$ We can use this expression in the equation for the center of mass. $\sum F = ma$ $mg-T = ma$ $mg - ma = ma$ $a = \frac{g}{2}$ We can find the angular acceleration. $\alpha = \frac{a}{R}$ $\alpha = \frac{g}{2R}$ $\alpha = \frac{9.80~m/s^2}{(2)(0.0800~m)}$ $\alpha = 61.25~rad/s^2$ We can find the angular position $\theta$ after the hoop has dropped a distance of 75.0 cm. $\theta = \frac{y}{R}$ $\theta = \frac{0.750~m}{0.0800~m}$ $\theta = 9.375~rad$ We can find the angular speed. $\omega^2 = \omega_0+2\alpha ~\theta$ $\omega = \sqrt{2\alpha ~\theta}$ $\omega = \sqrt{(2)(61.25~rad/s^2)(9.375~rad)}$ $\omega = 33.9~rad/s$ (b) We can find the speed of the center of mass. $v = \omega ~R$ $v = (33.9~rad/s)(0.0800~m)$ $v = 2.71~m/s$
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