Calibration
for
Network
Measurement
Two-P
ort Error
Model
The
error model
for
measurement
of
the
transmission
coecients
(magnitude
and
phase)
of
a
two-port device
is
derived
in
a
similar
manner
.
The
major
sources
of
error are
frequency
response
(tracking), source
match,
load
match,
and
isolation
(
Figure
A
-36
).
These
errors are
eectively
removed using
the
full
two-port
error
model
Figure
A
-36.
Major
Sources
of
Error
Measuring Transmission
Coecient.
The
transmission
coecient
is
measured
by
taking
the
ratio
of the
incident
signal
(I)
and
the
transmitted
signal
(T)
(
Figure
A
-37
).
Ideally
,
(I)
consists
only
of power
delivered
by
the
source
,
and
(T)
consists
only
of
power
emerging
at
the
test
device
output.
Figure A-37. Transmission Coecient
Load Match Error
.
As in the reection model, source match can
cause the incident signal to
vary as a function of test device S
11A
. Also
, because the test setup transmission return port is
never exactly the characteristic impedance
, some of the transmitted signal is reected from
the
test set port 2, and from other mismatches between the test device output and the receiver
input, to return to the test device. A portion of this signal may be re-reected at port 2, thus
aecting S
21M
, or part may be transmitted through the device in the reverse direction to
appear at port 1, thus aecting S
11M
. This error term, which causes the magnitude and phase
of the transmitted signal to vary as a function of S
22A
, is called load match, E
LF
(Figure A-38).
A-54 Basic Measurement Theory