Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 11 - Rolling, Torque, and Angular Momentum - Problems - Page 324: 51b

Answer

$\frac{2}{3}~~$ of the original rotational kinetic energy is lost.

Work Step by Step

Let $I_w$ be the rotational inertia of the first wheel. Then $2I_w$ is the rotational inertia of the second wheel. We can use conservation of angular momentum to find an expression for the angular speed of the resultant combination: $L_f = L_i$ $(I_w+2I_w)~\omega_f = I_w~\omega_i$ $3I_w~\omega_f = I_w~\omega_i$ $\omega_f =\frac{\omega_i}{3}$ We can write an expression for the initial rotational kinetic energy: $K_i = \frac{1}{2}I_w\omega_i^2$ We can write an expression for the new rotational kinetic energy: $K_f = \frac{1}{2}I_f\omega_f^2$ $K_f = \frac{1}{2}(3I_w)(\frac{\omega_i}{3})^2$ $K_f = \frac{1}{3}\times \frac{1}{2}I_w\omega_i^2$ $K_f = \frac{1}{3}~K_i$ Therefore, $~~\frac{2}{3}~~$ of the original rotational kinetic energy is lost.
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