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: 10.18

Answer

(a) $KE = 140~J$ (b) 33% of the kinetic energy is rotational kinetic energy.

Work Step by Step

(a) We can find the angular velocity. $\omega = (0.50~rev/s)(2\pi~rad/rev)$ $\omega = \pi~rad/s$ We can find the translational velocity. $v = \omega~R$ $v = (\pi~rad/s)(0.50~m)$ $v = (0.50~\pi)~m/s$ We can find the kinetic energy. $KE = \frac{1}{2}mv^2+\frac{1}{2}I\omega^2$ $KE = \frac{1}{2}mv^2+\frac{1}{2}(\frac{1}{2}mR^2)(\frac{v}{R})^2$ $KE = \frac{3}{4}mv^2$ $KE = \frac{3}{4}(75~kg)(0.50~pi~m/s)^2$ $KE = 140~J$ (b) The rotational energy is $\frac{1}{4}mv^2$. We can find the percent of the kinetic energy that is rotational kinetic energy. $\frac{KE_{rot}}{KE}\times 100\% =\frac{\frac{1}{4}mv^2}{\frac{3}{4}mv^2}\times 100\% = 33\%$ 33% of the kinetic energy is rotational kinetic energy.
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