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: 79

Answer

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Work Step by Step

a) We know, from simple systems, that the period is given by $$T=2\pi\sqrt{\dfrac{m}{k}}\tag 1$$ Solving for $k$; $$k=\dfrac{4\pi^2 m}{T^2}\tag 2$$ And since the period time $T$ will change by $dT$ when $m$ changes to $dm$, so taking the first derivative with respect to $m$ for (1). But first, we need to rewrite it as follows: $$T=2\pi k^{-\frac{1}{2}} (m)^{\frac{1}{2}}$$ where $T$ is a function in $m$ $$\dfrac{d}{dm}(T)=\dfrac{d}{dm}\left[2\pi k^{-\frac{1}{2}} (m)^{\frac{1}{2}} \right] $$ $$\dfrac{dT}{dm}= \color{red}{\bf\not} 2\pi k^{-\frac{1}{2}} \dfrac{1}{\color{red}{\bf\not} 2} (m)^{-\frac{1}{2}} $$ $$\dfrac{dT}{dm}= \pi k^{-\frac{1}{2}} (m)^{-\frac{1}{2}}=\dfrac{\pi}{\sqrt{km}} $$ Thus, $$ dT = \dfrac{\pi dm}{\sqrt{km}} $$ Plugging from (2); $$ dT =\dfrac{\pi dm}{\sqrt{\left[\dfrac{4\pi^2 m}{T^2}\right]m}} $$ $$ dT =\dfrac{\color{red}{\bf\not} \pi T dm}{ 2\color{red}{\bf\not} \pi m} $$ $$ \boxed{dT =\dfrac{ T dm}{ 2 m}} $$ Therefore, $$\boxed{ \Delta T =\dfrac{ T \Delta m}{ 2 m} }$$ --- b) The new period is given by $$T_{\rm new}=T+\Delta T$$ Plugging from the boxed formula above; $$T_{\rm new}=T+\dfrac{ T \Delta m}{ 2 m} $$ $$T_{\rm new}=T\left[1 +\dfrac{ \Delta m}{ 2 m} \right]$$ Plugging the known, where $\Delta m=0.1\% m=\dfrac{0.1}{100}m$ $$T_{\rm new}=2.0\left[1 +\dfrac{ 10^{-3}\color{red}{\bf\not} m}{ 2 \color{red}{\bf\not} m} \right]$$ $$T_{\rm new}=\color{red}{\bf 2.001}\;\rm s$$
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