Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 12 - Rotation of a Rigid Body - Conceptual Questions - Page 347: 2

Answer

$\sqrt 2\;R$

Work Step by Step

We know that rotational energy is given by $$K=\frac{1}{2}I\omega^2$$ So we need to double this energy without changing the angular velocity $\omega$. This means that we need to change the moment of inertia. $$K_f = \frac{1}{2}I_f\omega^2 $$ Since $K_f=2K$, then $$ \color{red}{\bf\not} \frac{1}{2}I_f\color{red}{\bf\not} \omega^2=2\times \color{red}{\bf\not} \frac{1}{2}I\color{red}{\bf\not} \omega^2$$ Thus, $$I_f=2I\tag 1$$ This means that we need to double the moment of inertia of the given object. And we also know that the moment of inertia is given by $$I=\int r^2dm$$ which means that $I\propto r^2$; and for our case, $$\dfrac{I}{I_f}=\dfrac{R^2}{R^2_f}$$ Plugging from (1); $$\dfrac{\color{red}{\bf\not} I}{2\color{red}{\bf\not} I}=\dfrac{R^2}{R^2_f}$$ Hence, $$R^2_f=2R$$ Thus, $$\boxed{R_f=\sqrt2 R}$$ Therefore, $R$ must e increased by a factor of $\sqrt2$
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