Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 16 - Waves-I - Problems - Page 474: 42a

Answer

$2f_3$

Work Step by Step

A string under tension $\tau_i$ oscillates in the third harmonic at frequency $f_3$, and the waves on the string have wavelength $\lambda_3$ Therefore, $f_3=\frac{v}{\lambda_3}$ or, $f_3=\frac{1}{\lambda_3}\sqrt {\frac{\tau_i}{\mu}}$ or, $\lambda_3=\frac{1}{f_3}\sqrt {\frac{\tau_i}{\mu}}$ If the tension is increased to $\tau_f=4\tau_i$ and the string is again made to oscillate in the third harmonic, then the frequency of oscillation is given by $f_3^{'}=\frac{1}{\lambda_3}\sqrt {\frac{\tau_f}{\mu}}$ $f_3^{'}=\frac{1}{\frac{1}{f_3}\sqrt {\frac{\tau_i}{\mu}}}\sqrt {\frac{4\tau_i}{\mu}}$ or, $f_3^{'}=2f_3$ $\therefore$ The frequency of oscillation is $2f_3$
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