College Physics (4th Edition)

Published by McGraw-Hill Education
ISBN 10: 0073512141
ISBN 13: 978-0-07351-214-3

Chapter 12 - Problems - Page 463: 16

Answer

The displacement amplitude is $2.77\times 10^{-7}~m$ The displacement amplitude is about 92 times larger than the average distance between molecules in a room.

Work Step by Step

We can find the intensity of the sound: $\beta = 10~log\frac{I}{I_0}$ $60.0 = 10~log\frac{I}{I_0}$ $6.0 = log\frac{I}{I_0}$ $10^{6.0} = \frac{I}{I_0}$ $I = (10^{6.0})~I_0$ $I = (10^{6.0})~(1.0\times 10^{-12}~W/m^2)$ $I = 1.0\times 10^{-6}~W/m^2$ We can use $343~m/s$ as the speed of sound in air. We can use $\rho = 1.2~kg/m^3$ as the density of air. We can find the displacement amplitude: $s_0 = \sqrt{\frac{I}{2\pi^2 \rho f^2 v}}$ $s_0 = \sqrt{\frac{1.0\times 10^{-6}~W/m^2}{(2\pi^2)(1.2~kg/m^3)(40~Hz)^2(343~m/s)}}$ $s_0 = 2.77\times 10^{-7}~m$ The displacement amplitude is $2.77\times 10^{-7}~m$ We can compare the displacement amplitude to $3~nm$: $\frac{2.77\times 10^{-7}~m}{3\times 10^{-9}~m} = 92$ The displacement amplitude is about 92 times larger than the average distance between molecules in a room.
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