Engineering Mechanics: Statics & Dynamics (14th Edition)

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

Chapter 14 - Kinetics of a Particle: Work and Energy - Section 14.3 - Principle of Work and Energy for a System of Particles - Problems - Page 198: 16

Answer

$41.4^{\circ}$

Work Step by Step

We can determine the required angle $\theta$ as follows: We know that $\Delta KE=\Delta PE$ $\implies \frac{1}{2}m_2^2-\frac{1}{2}mv_1^2=-mg(rcos\theta-r)$ This simplifies to: $v_2^2=2gr(\frac{9}{8}-cos\theta)$ As $a_{u_n}=\frac{v_2^2}{r}$ $\implies a_{u_n}=\frac{2gr(\frac{9}{8}-cos\theta)}{r}=2g(\frac{9}{8}-cos\theta)$ Now $F_N=mgcos\theta-ma_{u_n}$ $\implies F_N=mgcos\theta-m(2g(\frac{9}{8}-cos\theta))$ This simplifies to: $F_N=mg(3cos\theta-\frac{9}{4})$ $\implies 0=mg(3cos\theta-\frac{9}{4})$ This simplifies to: $\implies \theta=41.4^{\circ}$
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