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Wave Scattering by a Mass on a String

We have derived the reflectance and transmittance of a mass $ m$ as seen from either string at impedance $ R$. We can now derive the complete scattering relations:

For force waves, the outgoing waves are

\begin{eqnarray*}
F^{-}_1(s) &=& \hat{\rho}(s) F^{+}_1(s) + \hat{\tau}_f(s) F^{-...
...}_2(s) &=& \hat{\tau}_f(s) F^{+}_1(s) + \hat{\rho}(s) F^{-}_2(s)
\end{eqnarray*}

where the incoming waves are $ F^{+}_1$ and $ F^{-}_2$, and

\begin{eqnarray*}
\hat{\rho}(s)&=&\frac{ms}{ms+2R} \quad \mbox{(force reflectanc...
...{\rho}(s)=\frac{2(ms+R)}{ms+2R}\quad \mbox{(force transmittance)}\end{eqnarray*}

We may say that the mass creates a dynamic scattering junction on the string


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Download MassString.pdf
Download MassString_2up.pdf
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``Ideal Mass Colliding with an Ideal String'', by Julius O. Smith III, (From Lecture Overheads, Music 420).
Copyright © 2007-03-01 by Julius O. Smith III
Center for Computer Research in Music and Acoustics (CCRMA),   Stanford University
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