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: 10.45

Answer

(a) $\omega_2 = 1.38~rad/s$ (b) $K_1 = 1080~J$ $K_2 = 495~J$ These two kinetic energies are not equal because it required work to make the disk and parachutist rotate with the same angular speed.

Work Step by Step

(a) We can use conservation of angular momentum to solve this question. Let $M$ be the mass of the disk and let $m$ be the mass of the parachutist. $L_2 = L_1$ $I_2\omega_2 = I_1\omega_1$ $(\frac{1}{2}MR^2+mR^2)\omega_2 = \frac{1}{2}MR^2\omega_1$ $(M+2m)\omega_2 = M\omega_1$ $\omega_2 = \frac{M\omega_1}{M+2m}$ $\omega_2 = \frac{(120~kg)(3.00~rad/s)}{(120~kg)+(2)(70.0~kg)}$ $\omega_2 = 1.38~rad/s$ (b) We can find the initial kinetic energy. $K_1 = \frac{1}{2}I_1\omega_1^2$ $K_1 = \frac{1}{2}(\frac{1}{2}MR^2)\omega_1^2$ $K_1 = \frac{1}{4}(120~kg)(2.00~m)^2(3.00~rad/s)^2$ $K_1 = 1080~J$ We can find the final kinetic energy. $K_2 = \frac{1}{2}I_2\omega_2^2$ $K_2 = \frac{1}{2}(\frac{1}{2}MR^2+mR^2)\omega_2^2$ $K_2 = \frac{1}{2}[(\frac{1}{2})(120~kg)(2.00~m)^2+(70.0~kg)(2.00~m)^2](1.38~rad/s)^2$ $K_2 = 495~J$ These two kinetic energies are not equal because it required work to make the disk and parachutist rotate with the same angular speed.
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