Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 12 - Equilibrium and Elasticity - Problems - Page 353: 78a

Answer

$F = (-671~\hat{j})~N$

Work Step by Step

To find the gravitational force on the beam, we can consider the torque about the rotation axis at the hinge: $\sum \tau = 0$ $(L~cos~\theta)(400~N)-(\frac{L}{2}~sin~\theta)~(mg) = 0$ $(\frac{L}{2}~sin~\theta)~(mg) = (L~cos~\theta)(400~N)$ $mg = (2)(cot~\theta)(400~N)$ $mg = (2)(cot~50.0^{\circ})(400~N)$ $mg = 671~N$ The gravitational force on the beam is $~~671~N~~$ and this is directed downward. We can express the gravitational force on the beam in unit-vector notation: $F = (-671~\hat{j})~N$
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