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Operating Information
82
N432A User’s Guide
Voltage Standing Wave Ratio (VSWR) Measurement
This section describes how to measure the VSWR of a source which is the
reference oscillator/power reference connector on a power
meter- under- test.
When RF power is transferred from a source to a load, the level of power
absorbed by the load, P
A
, is dependent on the respective impedance of the
load and the respective output impedance of the source. This can be
expressed in terms of voltage reflection coefficients (VRCs) as follows:
where:
•
P
ZO
is the power that the source will deliver to a matched load.
•
Γ
S
and
Γ
L
are the VRCs of the source and load respectively.
This method for measuring the source match exploits this relationship by
presenting the source with two different values of
Γ
L
and measuring the
power delivered to the load under the two conditions. The load used is a
thermistor sensor that can be operated at two different resistances of
100
Ω
and 200
Ω
and can accurately measure the power absorbed. The
Keysight 478A thermistor sensor with Option H63, Option H75, or
Option H76 normally operates at a DC resistance of 200
Ω
giving an RF
impedance of 50
Ω
and
Γ
L
close to zero. When the thermistor bridge is set
to 100
Ω
, the RF impedance is 25
Ω
giving a nominal
Γ
L
of 0.33. The
correction factor/effective efficiency of the sensor remains constant under
these two conditions so that the power ratio between operation at 200
Ω
and 100
Ω
can be accurately measured.
If the two reflection coefficients are
Γ
1
and
Γ
2
and these give the power
measurements of P
1
and P
2
respectively (but the available power remains
the same) then the two relationships can be equated as follows:
P
A
P
ZO
1
Γ
L
2
–
1
Γ
s
Γ
L
–
2
----------------------------
×
=
P
1
1
Γ
s
Γ
1
–
2
1
Γ
1
2
–
---------------------------
P
2
1
Γ
s
Γ
2
–
2
1
Γ
2
2
–
---------------------------
=
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