Loop Attenuation at frequency $ f_1$

The gain of the low-pass filter at frequency $ f$ is

$\displaystyle G_a(f) = \cos(\pi fT_s).
$

After $ M$ passes through the delay-line loop, a partial at frequency $ f$ is subject to attenuation

$\displaystyle \cos(\pi fT_s)^M.
$

Since the round-trip time in the loop is $ N+1/2$ samples, the number of trips through the loop after $ n$ samples ($ n = tf_s$) is given by

$\displaystyle M = \frac{n}{N + 1/2} = \frac{tf_s}{N + 1/2}= tf_1.
$

The attenuation factor at time $ t=nT_s$ is given by

$\displaystyle \alpha_f(t) \triangleq \cos(\pi fT_s)^{tf_1}.
$

That is, a partial or harmonic of frequency $ f$, having an initial amplitude of $ A$ at time 0, will have amplitude $ A\alpha_f(t)$ at time $ t$ seconds.


``Music 206: Introduction to Delay and Filters II'' by Tamara Smyth, Computing Science, Simon Fraser University.
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Copyright © 2019-04-18 by Tamara Smyth.
Please email errata, comments, and suggestions to Tamara Smyth<trsmyth@ucsd.edu>