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 21 - Superposition - Exercises and Problems - Page 622: 33

Answer

$1.41\;\rm cm$

Work Step by Step

Since the string vibrates at its fundamental frequency, the wavelength of the standing wave is then equal to twice the length of the string; $(\lambda=2L)$. Recalling that the amplitude is given by $$A_{(x)}=2a\sin(kx)$$ where $k=\frac{2\pi}{\lambda}=\frac{2\pi}{2L}=\frac{\pi}{L}$ $$A_{(x)}=2a\sin\left(\dfrac{\pi x}{L}\right)$$ At $x=\frac{1}{4}L$, $A=2$ cm, so $$\color{red}{\bf\not} 2=\color{red}{\bf\not} 2a\sin\left(\dfrac{\pi \cdot\frac{1}{4}\color{red}{\bf\not} L}{\color{red}{\bf\not} L}\right)$$ $$a\sin\left(\frac{\pi}{4}\right)=1$$ Hence, $$a=\dfrac{1}{\sin\left(\frac{\pi}{4}\right)}=\sqrt{2}$$ $$a=\color{red}{\bf1.41}\;\rm cm$$
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