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Velocity Projection

The Doppler effect depends only on velocity components along the line connecting the source and listener.

We may therefore orthogonally project the source and listener velocities onto the vector $ \underline{x}_{sl}=\underline{x}_l-\underline{x}_s$ pointing from the source to the listener.

\begin{figure}\centering
\input fig/fhorn100.pstex_t
\\ {\LARGE Relevant geometry for a rotating horn}
\end{figure}


Projected source velocity:

\begin{eqnarray*}
\underline{v}_{sl}&=& {\cal P}_{\underline{x}_{sl}}(\underline...
...{x}_l\,\right\Vert\gg\left\Vert\,\underline{x}_s\,\right\Vert$)}
\end{eqnarray*}


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Download DelayVar.pdf
Download DelayVar_2up.pdf
Download DelayVar_4up.pdf

``Time Varying Delay Effects'', by Julius O. Smith III, (From Lecture Overheads, Music 420).
Copyright © 2008-02-08 by Julius O. Smith III
Center for Computer Research in Music and Acoustics (CCRMA),   Stanford University
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