
52 Electrotechnical Systems
is called the characteristic (wave) impedance. Under R = 0
Z
L
C
c
=
(2.20)
The general equations for currents and voltages in the transmission line are
IxsA A
(, ) =+
−
(2.21)
VxsZAZA
c
x
c
x
(, ) =− +
−
e e
(2.22)
where
s is the Laplace transformation symbol
x is the distance from the sending line end to the considered point
then the second terms are interpreted as the incident (forward) waves I
f
, V
f
, and the
rst terms are interpreted as the reected waves I
b
, V
b
. It is worth noting that the
distance x is taken often from the receiving line end [2]; in this case, signs by γ in
(2.21), (2.22) change. If the line is loaded ...