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 331: 10.27

Answer

(a) At the base of the hill, it was rotating at a rate of 67.9 rad/s. (b) $K_{rot} = 8.36~J$

Work Step by Step

(a) We can use conservation of energy to solve this question. The potential energy at the top will be equal to the total kinetic energy at the bottom. $\frac{1}{2}mv^2+\frac{1}{2}I\omega^2 = mgh$ $\frac{1}{2}mv^2+\frac{1}{2}(\frac{2mR^2}{3})(\frac{v}{R})^2 = mgh$ $\frac{1}{2}v^2+\frac{1}{3}v^2 = gh$ $v^2 = \frac{6gh}{5}$ $v = \sqrt{\frac{6gh}{5}}$ $v = \sqrt{\frac{(6)(9.80~m/s^2)(5.00~m)}{5}}$ $v = 7.67~m/s$ We can use the velocity to find the angular velocity. $\omega = \frac{v}{R}$ $\omega = \frac{7.67~m/s}{0.113~m}$ $\omega = 67.9~rad/s$ At the base of the hill, it was rotating at a rate of 67.9 rad/s. (b) We can find the rotational kinetic energy. $K_{rot} = \frac{1}{2}I\omega^2$ $K_{rot} = \frac{1}{2}(\frac{2mR^2}{3})\omega^2$ $K_{rot} = \frac{1}{3}(mR^2)\omega^2$ $K_{rot} = \frac{1}{3}(0.426~kg)(0.113~m)^2(67.9~rad/s)^2$ $K_{rot} = 8.36~J$
Update this answer!

You can help us out by revising, improving and updating this answer.

Update this answer

After you claim an answer you’ll have 24 hours to send in a draft. An editor will review the submission and either publish your submission or provide feedback.