41Theory of Distributed-Parameter Circuits and Impedance
IYVdx=−
∫
(1.118)
For a semi-innite line, substituting the rst equation of Equation 1.112
into Equation 1.118 gives
IYPPxVYPV
f
=−−−=
−−
()exp()
///121212
(1.119)
Therefore, the characteristic impedance and admittance matrices are
found as
ZPYYYP
0
121
0
12
==
−−//
,(1.120)
This equation produces the same matrices as in Equation 1.113. For exam-
ple, for the characteristic admittance matrix:
YYPPYPPYPZYY
0
121112111211121
====
−−−−−−−−
−−
(())()()((
))
//
//
−−
−
−
−
=
(
)
=
1
12
1
112
PZZP
//
(1.121)
The characteristic impedance and admittance matrices are symmetrical
matrices. For example, for the characteristic impedance matrix:
ZPYYPY
PZ
ttttt0
121112112
0
====
−−−
()
///
(1.122)
Here, Y = Y
t
since Y is a symmet ...
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