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 405: 67

Answer

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Work Step by Step

a) We know that the frequency of an object that undergoes a simple harmonic motion is given by $$f=\dfrac{1}{2\pi}\sqrt{\dfrac{k}{m}}$$ where $k$ is the spring constant and $m$ is the object's mass. So the spring constant is found by squaring both sides and then solving for $k$; $$4\pi^2 f^2=\dfrac{k}{m}$$ $$k=4\pi^2 f^2 m$$ Plugging the known; $$k=4\pi^2 (4.0)^2 (15\times 10^{-3})$$ $$k=\color{red}{\bf 9.475}\;\rm N/m$$ --- b) In damping oscillations, we know that the amplitude is given by $$x_{(t)}=A_0e^{-t/2\tau}$$ where $\tau= m/b$, so $$x_{(t)}=A_0e^{-bt/2m}$$ where $b$ is the damping constant we need to find. So, $$\dfrac{x_{(t)}}{A_0}=e^{-bt/2m}$$ $$\ln\left[ \dfrac{x_{(t)}}{A_0} \right]=\dfrac{-bt}{2m}$$ Hence, $$b=-\left(\dfrac{2 m}{t}\right)\ln\left[ \dfrac{x_{(t)}}{A_0} \right] \tag 1$$ The author here did not tell us the initial amplitude so we can't find the magnitude of $b$. But yet we can plug the known; $$ b=-\left(\dfrac{ 2(15\times 10^{-3})}{4}\right)\ln\left[ \dfrac{(0.5\times 10^{-2})}{A_0} \right] $$ Let's assume that $A_0=4$ cm, so $$ b=-\left(\dfrac{ 30\times 10^{-3}}{4}\right)\ln\left[ \dfrac{(0.5\times 10^{-2})}{(4\times 10^{-2})} \right] $$ $$b=\bf 15.6\times 10^{-3}\;\rm kg/s$$
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