Sampled Travelling Waves

Sampling is carried out by the change of variables

$\displaystyle x \rightarrow x_m$ $\displaystyle =$ $\displaystyle mX$  
$\displaystyle t \rightarrow t_n$ $\displaystyle =$ $\displaystyle nT,$  

where $ T$ is the temporal sampling interval, and $ X \triangleq cT$, is the spatial sampling interval

Substituting into the traveling-wave solution yields

$\displaystyle y(t_n,x_m)$ $\displaystyle =$ $\displaystyle y_r(t_n- x_m/c) + y_l(t_n+ x_m/c)$  
  $\displaystyle =$ $\displaystyle y_r(nT- mX/c) + y_l(nT+ mX/c)$  
  $\displaystyle =$ $\displaystyle y_r\left[(n-m)T\right]+ y_l\left[(n+m)T\right]$  

Since $ T$ multiplies all arguments it is typically suppressed.

This notation is also used to model pressure in acoustic tubes.


``Music 206: Digital Waveguides'' by Tamara Smyth, Department of Music, University of California, San Diego (UCSD).
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Copyright © 2019-05-01 by Tamara Smyth.
Please email errata, comments, and suggestions to Tamara Smyth<trsmyth@ucsd.edu>