Physics (10th Edition)

Published by Wiley
ISBN 10: 1118486897
ISBN 13: 978-1-11848-689-4

Chapter 9 - Rotational Dynamics - Problems - Page 250: 83

Answer

The thin-walled spherical shell has greater moment of inertia. Its deceleration is smaller and therefore, it takes a longer time for that shell to come to a halt. The time it takes for the solid sphere to stop: $t_1=4.8s$ The time it takes for the thin-walled sphere to stop: $t_1=8s$

Work Step by Step

i) From Table 9.1, a solid sphere with axis through center has $I=2/5MR^2$, while a thin-walled sphere with axis through the center has $I=2/3MR^2$. Therefore, the thin-walled spherical shell has greater moment of inertia. ii) The torque produced by friction will cause the sphere to decelerate, following the equation: $$\tau=I\alpha$$ Because the thin-walled shell has greater $I$, the magnitude of its deceleration will be smaller. iii) Because the magnitude of the thin-walled shell's deceleration is smaller, it will take a longer time for the thin-walled shell to come to a halt. The deceleration of each sphere is: - Solid sphere: $$\alpha_1=\frac{-\tau}{\frac{2}{5}MR^2}=\frac{-0.12N.m}{\frac{2}{5}(1.5kg)(0.2m)^2}=-5rad/s^2$$ - Thin-walled sphere: $$\alpha_2=\frac{-\tau}{\frac{2}{3}MR^2}=\frac{-0.12N.m}{\frac{2}{3}(1.5kg)(0.2m)^2}=-3rad/s^2$$ The time it takes for each sphere to stop is - Solid sphere: $$t=\frac{\omega-\omega_0}{\alpha_1}=\frac{0-24rad/s}{-5rad/s^2}=4.8s$$ - Thin-walled sphere: $$t=\frac{\omega-\omega_0}{\alpha_2}=\frac{0-24rad/s}{-3rad/s^2}=8s$$
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