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The Doppler Effect

In the real world, a Doppler shift is an apparent change in acoustic frequency content of a sound source due to motion of the source relative to the listener. You have probably heard the pitch of a horn drop lower as it passes by (e.g., from a moving train). While a pitched sound-source is moving toward the listener, the heard pitch is higher than it is at rest; while the source is moving away from the listener, its pitch is lowered.

As derived in elementary physics texts, the Doppler shift is given by

$\displaystyle \omega_l = \omega_s \frac{1+\frac{v_{ls}}{c}}{1-\frac{v_{s,l}}{c}} \protect$ (1)

where $ \omega_s $ is the radian frequency emitted by the source at rest, $ \omega_l $ is the frequency received by the listener, $ v_{ls}$ denotes the speed of the listener relative to the propagation medium in the direction of the source, $ v_{s,l}$ denotes the speed of the source relative to the propagation medium in the direction of the listener, and $ c$ denotes sound speed. Note that all quantities in this formula are scalars.



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``Doppler Simulation and the Leslie'', by Julius O. Smith III, Stefania Serafin, Jonathan Abel, David P. Berners, Music 421 Handout, Spring 2002 .
Copyright © 2016-03-26 by Julius O. Smith III, Stefania Serafin, Jonathan Abel, David P. Berners
Center for Computer Research in Music and Acoustics (CCRMA),   Stanford University
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