Physics (10th Edition)

Published by Wiley
ISBN 10: 1118486897
ISBN 13: 978-1-11848-689-4

Chapter 10 - Simple Harmonic Motion and Elasticity - Problems - Page 279: 76

Answer

0.13 m

Work Step by Step

By combining equations 10.5, 10.16 we can get, $\frac{2\pi}{T}=\sqrt {\frac{g}{L}}$ ; Solving for the length L, we get, $L=\frac{T^{2}g}{4\pi^{2}}$ Difference between the final and initial = $L_{2}-L_{1}$ $L_{2}-L_{1}=\frac{T_{2}^{2}g}{4\pi^{2}}-\frac{T_{1}^{2}g}{4\pi^{2}}=\frac{(T_{2}^{2}-T_{1}^{2})g}{4\pi^{2}}$ $L_{2}-L_{1}=[(1.45\space s)^{2}-(1.25\space s)^{2}]\frac{9.8\space m/s^{2}}{4\pi^{2}}\approx0.13\space m$
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