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Backward Difference Conformal Map

We saw that the backwards difference substitution can be seen as a conformal map taking the $ s$ plane to the $ z$ plane:

$\displaystyle \zbox{s\to \frac{1-z^{-1}}{T}}
$

Look at the image of the $ j\omega$ axis under this mapping:

\epsfbox{eps/freqmap.eps}

The continuous-time frequency axis, $ s=j\omega$ , is not mapped to the discrete-time frequency axis (unit circle):

This means artificial damping will be introduced for high-frequency system resonances


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Download DigitizingNewton.pdf
Download DigitizingNewton_2up.pdf
Download DigitizingNewton_4up.pdf

``Introduction to Physical Signal Models'', by Julius O. Smith III, (From Lecture Overheads, Music 420).
Copyright © 2020-06-27 by Julius O. Smith III
Center for Computer Research in Music and Acoustics (CCRMA),   Stanford University
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