
Antennas and Microwaves

Balanced Measurements
The Theory
There many instances in RF and antenna work where a balanced transmission line or radiating element is used. Creating a physical balun so that measurements can be made on a single ended system is one option. However, the physical realisation is seldom ideal over the frequency range of interest and often just adds uncertainty to the results.
Another option is to calculate the balanced impedance from 2 single ended measurements.
The derivation of the balanced line impedance presented here takes an intuitive approach
to the problem, see figure 1 below. The unbalanced system is a standard 2-
The reflection coefficient, Rho is defined as the (return signal) / (incident signal).
For the unbalanced system this is just S11. For the balanced system the reflection
coefficient simplifies to (S11-
Having established the reflection coefficients Rho(bal1) and Rho(bal2) for each arm
of the system, the input impedance is readily calculated using Zin=((1+Rho)/(1-
Replacing -
Where (Theta) in radians represents the angle between the excitation phases.
Theta = pi balanced feed
Theta = pi/2 quadrature fed
Theta = pi co-

Figure1
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Practical Measurement
In order to make practical use of this result the device under test (DUT) has to
be characterised with a full set of s-
Note that the S-
To make the system as near 'real-


