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Example: Leaky Integrator

\begin{eqnarray*}
H_a(s) &=& \frac{1}{s+\epsilon } \;\longrightarrow\;
H_d(z) \;=\;\frac{1}{\frac{1+\alpha}{T}\frac{1-z^{-1}}{1+\alpha\,z^{-1}}+\epsilon }\\ [5pt]
&=& g \frac{1+\alpha z^{-1}}{1-pz^{-1}},\quad
\zbox{p = \frac{1-\alpha\frac{\epsilon T}{1+\alpha}}{1+\frac{\epsilon T}{1+\alpha}}}, \quad
g = \frac{T}{1+\alpha+\epsilon T}
\end{eqnarray*}


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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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