Essential University Physics: Volume 1 (4th Edition)

Published by Pearson
ISBN 10: 0-134-98855-8
ISBN 13: 978-0-13498-855-9

Chapter 12 - Exercises and Problems - Page 224: 41

Answer

$\frac{1}{2}Mg(\sqrt {L^{2}+D^{2}}-L)$

Work Step by Step

Please see the attached image first, By using the principle of Pythagoras, $AB^{2}=L^{2}+D^{2}$ $AB=\sqrt {L^{2}+D^{2}}-(1)$ Energy provided $(E)=$Final potential energy - Initial potential energy $E=Mg\frac{(AB)}{2}-Mg\frac{L}{2}$ $(1)=\gt$ $E=\frac{Mg}{2}(\sqrt {L^{2}+D^{2}}-\frac{MgL}{2})$ $E=\frac{1}{2}Mg(\sqrt {L^{2}+D^{2}}-L)$ The energy needed to bring the pipe $=E=\frac{1}{2}Mg(\sqrt {L^{2}+D^{2}}-L)$ to the adjacent unstable equilibrium
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