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Lossless Scattering
The delay-line inputs (outgoing traveling waves) are computed by
multiplying the delay-line outputs (incoming traveling waves) by the
feedback matrix (scattering matrix)
. By
defining
,
, we obtain the more
usual DWN notation
 |
(C.119) |
where

is the vector of incoming traveling-wave samples
arriving at the junction at time

,

is the vector of
outgoing traveling-wave samples leaving the junction at time

, and

is the
scattering matrix associated with the
waveguide
junction.
The junction of
physical waveguides determines the structure of the
matrix
according to the basic principles of physics.
Considering the parallel junction of
lossless acoustic tubes, each
having characteristic admittance
, the continuity of pressure and
conservation of volume velocity at the junction give us the following
scattering matrix for the pressure waves [433]:
![$\displaystyle {\bf A} = \left[ \begin{array}{rrrr} \frac{2 \Gamma_{1}}{\Gamma_J...
...{2}}{\Gamma_J} & \dots & \frac{2 \Gamma_{N}}{\Gamma_J} -1\\ \end{array} \right]$](http://www.dsprelated.com/josimages_new/pasp/img4059.png) |
(C.120) |
where
 |
(C.121) |
Equation (
C.121) can be derived by first writing the
volume velocity at the

-th tube in terms of pressure waves as

.
Applying the conservation of velocity we can find the expression
for the junction pressure. Finally, if we express the junction
pressure as the sum of incoming and outgoing pressure waves at any
branch, we derive (
C.121). See §
C.12 for further
details.
Previous: FDNs as Digital Waveguide NetworksNext: Normalized Scattering
About the Author: 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.