Engineering Mechanics: Statics & Dynamics (14th Edition)

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

Chapter 17 - Planar Kinetics of a Rigid Body: Force and Acceleration - Section 17.3 - Equations of Motion: Translation - Problems - Page 439: 44

Answer

$\theta=tan^{-1}(\frac{a}{g})$

Work Step by Step

We can determine the required angle as follows: $\Sigma F_x=ma_x$ $\implies A_x=-ma$ Similarly, the equation of motion in y-direction is given as $\Sigma F_y=ma_y$ $\implies A_y-W=0$ $\implies A_y=mg$ Now, we apply the sum of moment about the center of gravity $\Sigma M_G=0$ $\implies -A_x(Lcos\theta)-A_y (Lsin\theta)=0$ $\implies -(-ma)Lcos\theta-mgLsin\theta=0$ $\implies acos\theta=gsin\theta$ This simplifies to: $tan\theta=\frac{a}{g}$ $\implies \theta=tan^{-1}(\frac{a}{g})$
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