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Lossy
Finite Difference Recursion
We will now derive a finite-difference model in terms of string
displacement samples which correspond to the lossy digital waveguide
model of Fig.H.5. This derivation generalizes the lossless case
considered in §H.4.3.
Figure H.7 depicts a digital waveguide section once again in
``physical canonical form,'' as shown earlier in Fig.H.5, and
introduces a doubly indexed notation for greater clarity in the
derivation below
[453,226,124,123].
Figure H.7:
Lossy digital waveguide--frequency-independent loss-factors
.
 |
Referring to Fig.H.7, we have the following time-update
relations:
Adding these equations gives
This is now in the form of the
finite-difference time-domain (FDTD)
scheme analyzed in [
226]:
with

, and

. In
[
124], it was shown by
von Neumann analysis
(§
N.4) that these parameter choices give rise to a stable
finite-difference scheme (§
N.2.3), provided

. In the
present context, we expect
stability to follow naturally from starting
with a passive digital waveguide model.
Subsections
Previous:
Digital Filter Models of Damped StringsNext:
Frequency-Dependent Losses
written by Julius Orion Smith III
Julius Smith's background is in electrical engineering (BS Rice 1975, PhD Stanford 1983). He is presently Professor of Music and Associate Professor (by courtesy) of Electrical Engineering at
Stanford's Center for Computer Research in Music and Acoustics (CCRMA), teaching courses and pursuing research related to signal processing applied to music and audio systems. See
http://ccrma.stanford.edu/~jos/ for details.