Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 14 - Oscillations - Exercises and Problems - Page 406: 70

Answer

$21\;\rm oscillation$

Work Step by Step

Our system undergoes a damping simple harmonic motion, so the maximum displacement is given by $$A_{(t)}=Ae^{−t/2\tau}$$ Hence, we need to find the time at which the final amplitude is $e^{-1} $ the initial amplitude. $$e^{-1}\color{red}{\bf\not} A =\color{red}{\bf\not} Ae^{−t/2\tau}$$ Thus, $$\dfrac{-t}{2\tau}=-1$$ $$t=2\tau=\dfrac{2m}{b}$$ $$t=\dfrac{2m}{b}\tag 1$$ Now we need to find the period of one full oscillation to find the number of oscillations after time interval of $t=33.33\;\rm s$. We know that the angular frequency of a damped oscillator is given by $$\omega=2\pi f=\sqrt{\dfrac{k}{m}-\dfrac{b^2}{4m^2}}$$ where $f=1/T$, so $$ \dfrac{2\pi}{T}=\sqrt{\dfrac{k}{m}-\dfrac{b^2}{4m^2}} $$ So, $$ T= \dfrac{2\pi}{\sqrt{\dfrac{k}{m}-\dfrac{b^2}{4m^2}} } \tag 2 $$ The number of oscillations is given by $$N=\dfrac{t}{T}$$ Plugging from (1) and (2); $$N=\dfrac{2m/b}{\dfrac{2\pi}{\sqrt{\dfrac{k}{m}-\dfrac{b^2}{4m^2}} } }$$ $$N=\dfrac{2m\sqrt{\dfrac{k}{m}-\dfrac{b^2}{4m^2}} }{ 2b\pi }$$ $$N=\dfrac{2m}{2b\pi }\sqrt{\dfrac{k}{m}-\dfrac{b^2}{4m^2}} $$ Plugging the known; $$N=\dfrac{2(0.250)}{2(0.015)\pi }\sqrt{\dfrac{4}{0.250}-\dfrac{(0.015)^2}{4(0.250)^2}}=\bf 21.22 $$ $$N\approx\color{red}{\bf 21}\;\rm oscillation$$ So it needs 21 oscillations to reach the amplitude to $e^{-1}A$.
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