Deriving the Reflection Coefficient

Figure 6: Scattering: a junction with another section.
\begin{figure}\centerline{%
\input{scattering.pstex_t}}\end{figure}

The relationship between the adjacent impedances causes a reflection in the first section that can be expressed in terms of tube area cross-sectional $ S$,

$\displaystyle R_1$ $\displaystyle =$ $\displaystyle \frac{p_1^{-}(J)}{p_1^{+}(J)}$  
  $\displaystyle =$ $\displaystyle \frac{Z_2 - Z_1}{Z_2 + Z_1}$  
  $\displaystyle =$ $\displaystyle \frac{S_1 - S_2}{S_1 + S_2} = k.$  

It follows that the reflection in the second section is

$\displaystyle R_2 = \frac{S_2 - S_1}{S_2 + S_1}- = -k.
$


``MUS 206: Modeling Acoustic Tubes and Wind Instrument Bores/Bells'' by Tamara Smyth, Department of Music, University of California, San Diego (UCSD).
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Copyright © 2019-05-22 by Tamara Smyth.
Please email errata, comments, and suggestions to Tamara Smyth<trsmyth@ucsd.edu>