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Two-Port Scattering Junctions

Force and velocity must be continuous at every point

\begin{eqnarray*}
f_{i-1}(t,cT) &=& f_i(t,0)
\\
v_{i-1}(t,cT) &=& v_i(t,0) \nonumber
\end{eqnarray*}

Velocity is positive to the right.
Stress (compression pressure or force density) is scalar.

Scattering relations:

\begin{eqnarray*}
f^{{+}}_i(t) &=& \left[1+k_i\right]f^{{+}}_{i-1}(t-T) - k_if^{...
...(t+T) &=& k_if^{{+}}_{i-1}(t-T) + \left[1-k_i\right]f^{{-}}_i(t)
\end{eqnarray*}

where

$\displaystyle \zbox{k_i\mathrel{\stackrel{\mathrm{\Delta}}{=}}\frac{ R_i-R_{i-1}}{R_i+R_{i-1}}}
$

is the $ i$th reflection coefficient (we'll derive this later as a special case of $ N$-port scattering)

\epsfig{file=eps/Fkl.eps,width=5in}

The Kelly-Lochbaum scattering junction


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Download Scattering.pdf
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``Scattering at an Impedance Discontinuity'', by Julius O. Smith III, (From Lecture Overheads, Music 420).
Copyright © 2007-05-14 by Julius O. Smith III
Center for Computer Research in Music and Acoustics (CCRMA),   Stanford University
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