Essential University Physics: Volume 1 (4th Edition)

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

Chapter 13 - Exercises and Problems - Page 246: 29

Answer

0.25 s

Work Step by Step

Here we use the equation, $x(t)=Ae^{\frac{-bt}{2m}}cos(\omega t+\theta)$; Where, x(t) - Displacement, A - Amplitude, $\omega $ -Angular velocity, t - time, b - constant, m - mass on the string, $\theta$ - Phase constant. $x(t)=Ae^{\frac{-bt}{2m}}cos(\omega t+\theta)-(1)$ When the amplitude drops to half its initial value, we can write, $e^{\frac{-bt}{2m}}=\frac{1}{2}$ Now Let's take the natural logarithm of both sides. $lne^{\frac{-bt}{2m}}=ln\frac{1}{2}=\gt \frac{-bt}{2m}=-0.7-(2)$ We know that the $\frac{b}{2m}=2.8\space s^{-1}=\gt(2)$ $2.8\space s^{-1}t=0.7$ $t=0.25\space s$ It will take 0.25 s amplitude to drop to half its original value.
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