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Reflection Coefficient, Parallel Case
The reflection coefficient seen at port
is defined as
 |
(F.20) |
In other words, the
reflection coefficient specifies what portion of
the incoming wave

is
reflected back to port

as
part of the outgoing wave

. The total outgoing wave on port

is the
superposition of the reflected wave and the

transmitted waves from the other ports:
 |
(F.21) |
where

denotes the
transmission coefficient from
port

to port

. Starting with Eq.

(
F.19) and substituting
Eq.

(
F.18) gives
Equating like terms with Eq.
(F.21), we obtain
Thus, the

th alpha parameter is the
force transmission coefficient
from

th port to any other port (besides the

th). To convert the
transmission coefficient from the

th port to the reflection
coefficient for that port, we simply subtract 1. This general
relationship is specific to
force waves at a parallel junction, as we
will soon see.
Previous: Alpha ParametersNext: Physical Derivation of Reflection Coefficient
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.