Engineering Mechanics: Statics & Dynamics (14th Edition)

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

Chapter 11 - Virtual Work - Section 11.3 - Principle of Virtual Work for a System of Connected Rigid Bodies - Problems - Page 594: 13

Answer

$\theta=90^{\circ}$, $\theta=36.1^{\circ}$

Work Step by Step

We can determine the required angle $\theta$ as follows: $\Sigma M_B=0$ $\implies \implies 2R_A(150-5)(9.81)(\frac{150+250}{2})-1(9.81)(400)=0$ $\implies R_A=45.78N$ and $\Sigma Y_i=0$ $\implies R_C(150)+5(9.81)+1(9.81)-45.78=0$ $\implies R_C=16.35N$ Now, the virtual displacements are given as $\delta_y=\frac{d(250 sin\theta)}{d\theta}=250 cos\theta$ and $\delta_x=\frac{d(250 cos\theta)}{d\theta}=-250 sin\theta$ According to the virtual-work equation $\delta U=0$ $\implies R_A\delta_{yA}-R_C\delta_{yC}+F_s\delta x_{c}=0$ We plug in the known values to obtain: $45(75)(250)cos\theta-16.35(250)cos\theta-50cos\theta(250) sin\theta=0$ This simplifies to: $\theta=36.1^{\circ}$
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