By
Mike Gibson and Ivor Catt, June 1986
Here
is a description of the symbols used in the derivations:
VFC voltage on cable moving towards the
inductor
VRC voltage on cable moving away from the
inductor
ZC characteristic impedance of the
cable
VFE voltage traveling in the forward
direction in the even mode
VFO voltage traveling in the forward
direction in the odd mode
VRE voltage traveling in the reverse
direction in the even mode
VRO voltage traveling in the reverse
direction in the odd mode
ZE characteristic impedance of even
mode
ZO characteristic impedance of odd mode
VFS secondary voltage moving away from the
transformer
VRS secondary voltage moving towards the
transformer
Going
from the cable to the inductor, the following basic equations hold,
1)
2)
3)
Transforming
(2) into voltages gives,
4)
Multiplying
through by ZC and defining new terms for the resulting ratios
yields,
5)
6)
From
(1),
7)
Substituting
(7) into (5) and gathering terms,
8)
From
(3), VFO = VFE . Substituting this into (8) gives,
8)
9)
Substituting
VFE and VFO from (8) and (9) into (7) gives
the reflection coefficient,
10)
Going
from the even and odd modes in the inductor to the cable, the following
equations hold,
1)
2)
3)
Reflection
coefficients can be derived using the same procedure as in the Cable to
Inductor section,
4)
5)
6)
7)
Using
these, the transmission coefficients to the cable can be derived,
8)
9)
Going
from the even and odd modes in the transformer to the secondary cable, the
following equations hold,
1)
2)
3)
Two
new ratios emerge in the derivation of the reflection and transmission
coefficients,
4)
The
resulting reflection coefficients are,
5)
6)
7)
8)
And
the resulting transmission coefficients are,
9)
10)
Going
from the secondary into the transformer, the following equations hold,
1)
2)
3)
1)
2)
3)