University of Cincinnati--ECE&CS Department
Impedance Concepts in Microwave Frequencies
Prepared by: Prof.Altan M. Ferendeci


Microwave Network Analysis


Given a series RLC circuit.

RLC Circuit

This has two terminals or a single port. It will be referred to as a one port network. Complex input power to this network is given by

Equation 1
Recalling the power dissipated in a resistor, the energy stored in an inductor and energy stored in a capacitor as

Equation 2
Equation 1 can be written as
Equation 3

Solving for Zin

Equation 4

If we were to consider an equivalent parallel RLC network, the input admittance can be written (with a derivation similar to the series circuit) as

 Admittance

A one port microwave network can be visualized by

Microwave One Port

There is only one input where fields can enter into and leave out of the system. Since this has only a single input, it will be refrerred to as a one port microwave network.

A reference plane is chosen at a specfic input location. At this reference plane, power into and out of the network can be calculated in terms of the field quantities. Within the network, there will be power dissipated due to the finite conductivity of the walls as well as the presence of lossy dielectric or magnetic materials. The electric and magnetic energies associated with the fields can also be computed. Therefore at the input port of a microwave network an equivalent one port input impedance can be defined similar to the RLC series (or parallel) network. The equivalent input impedance can be written similar to Eq. 3.

Lossles Impedance Note that associated with the Electric Field, we were able to write an equivalent travelling voltage wave for a transmission line. Also, associated with the magnetic field,an equivalent travelling current wave was written before. At the chosen terminal plane of the one-port network, these will have specific complex values. These are repesented in the figure above as
Vin=(V++V-) and Iin=(I+-I-)=(V+-V-)/Zc.
For the charateristic impedance:

Many microwave networks can be assumed to be lossless (small losses can be neglected), i.e., Pl=0. In this case, for a one port network, Eq.3 reduces to

Lossles Impedance

And for the parallel network

Lossles Admittance

Input reactance (or susceptance) can be zero if Wm=We. This is the resonance condition. It implies that either

Wm=We but (I.not.0): ( series resonance) or

Wm=We but (V.not.0): (parallel resonance).

The above concepts can be generalized to N-port networks.


Copyright; Altan M. Ferendeci, University of Cincinnati