D-1
APPENDIX D
Electrical length compensation
A test port extension can be modeled using a coaxial transmission line as shown in Figure D-1.
When an impedance element Z
L
is connected to the tip of the line, the measured impedance value Zi
at the other end of the line (that is, test port) is given by the following equation:
Z
L
+ Zo tan h γ
Zi = Zo ———————————
Z
L
tan h γ + Zo
γ = α + jβ = √ZY = √(R+jωL)(G+jωC)
Where, γ: Propagation constant of the transmission line
α: Attenuation constant of the transmission line
β: Phase constant of the transmission line
: Transmission line length
Zo: Characteristic impedance of the transmission line
Figure D-1. Transmission line model of test port extension
The DUT impedance value is therefore calculated as:
Zo tan h γ - Zi
Z
L
= Zo ———————————
Zi tan h γ - Zo
If the transmission line has no propagation loss (α=0, β=ω√LC
–––
), the equation for Z
L
is simplified as
follows:
Zi - jZo tan β
Z
L
= Z o —————————
Zo - jZi tan β
The true Z
L
value can be calculated if the phase shift quantity, β , is known. Here, the phase con-
stant β is related to the test signal wavelength γ in the transmission line as follows:
2π
β =
———
λ
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