Physics Technology Update (4th Edition)

Published by Pearson
ISBN 10: 0-32190-308-0
ISBN 13: 978-0-32190-308-2

Chapter 14 - Waves and Sound - Problems and Conceptual Exercises - Page 497: 116

Answer

(a) $257Hz; 255Hz$ (b) $2Hz$ (c) $0.670m$ (d) $2.0Hz$

Work Step by Step

(a) When the observer is moving towards the speaker, the frequency is given as $f_1=(1+\frac{u}{v})f$ We plug in the known values to obtain: $f_1=(1+\frac{1.35m/s}{342m/s})(256Hz)$ $\implies f_1=257Hz$ If the observer is moving away from the sound speaker, then the frequency can be determined as $f_2=(1-\frac{u}{v})f$ We plug in the known values to obtain: $f_2=(1-\frac{1.35m/s}{343m/s})(256Hz)$ $f_2=255hz$ (b) The beat frequency heard by the observer can be determine as $f^{\prime}=f_1-f_2$ We plug in the known values to obtain: $f^{\prime}=257Hz-255HZ$ $\implies f^{\prime}=2Hz$ (c) We know that $d=\frac{1}{2}(\frac{v}{f})$ $\implies d=\frac{1}{2}(\frac{343m/s}{256Hz})$ $d=0.670m$ (d) We know that $t=\frac{d}{u}$ $t=\frac{0.670m}{1.35 m/s}$ $t=0.5s$ and $\Delta f=\frac{1}{t}$ $\Delta f=\frac{1}{0.5s}=2.0Hz$ Thus, the observer hears the maximum loudness from the speaker 2 times per second and this is equal to the beat frequency.
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