Engineering Mechanics: Statics & Dynamics (14th Edition)

Published by Pearson
ISBN 10: 0133915425
ISBN 13: 978-0-13391-542-6

Chapter 15 - Kinetics of a Particle: Impulse and Momentum - Section 15.7 - Principle of Angular Impulse and Momentum - Problems - Page 292: 104

Answer

$r_2=1.52ft$, $t=0.74s$

Work Step by Step

The required time and distance can be determined as follows: We know that $v_2=\sqrt{(v_{\theta})_2^2+(v_r)_2^2}$ $12=\sqrt{(v_{\theta})^2+(2)^2}$ $\implies v_{\theta}=11.83ft/s$ According to the conservation of angular momentum $m_B(v_B)_1r_1=m_B(v_{\theta})r_2$ $\implies 6\times 3=11.83r_2$ $\implies r_2=1.52ft$ Now, $t=\frac{\Delta r}{v_r}$ We plug in the known values to obtain: $t=\frac{3-1.52}{2}$ This simplifies to: $t=0.74s$
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