Image impedance

Image impedance is a concept used in electronic network design and analysis and most especially in filter design. The term image impedance applies to the impedance seen looking in to the ports of a network. Usually a two-port network is implied but the concept is capable of being extended to networks with more than two ports. The definition of image impedance for a two-port network is the impedance, Z_{i 1}, seen looking in to port 1 when port 2 is terminated with the image impedance, Z_{i 2}, for port 2. In general, the image impedances of ports 1 and 2 will not be equal unless the network is symmetrical (or anti-symmetrical) with respect to the ports.__TOC__

Derivation

As an example, the derivation of the image impedances of a simple 'L' network is given below. The L network consists of a series impedance Z and a shunt admittance Y.

The difficulty here is that in order to find Z_{i 1} it is first necessary to terminate port 2 with Z_{i 2}. However, Z_{i 2} is also an unknown at this stage. The problem is solved by terminating port 2 with an identical network, port 2 of the second network is connected to port 2 of the first network and port 1 of the second network is terminated with Z_{i 1}. The second network is terminating the first network in Z_{i 2} as required. Mathematically, this is equivalent to eliminating one variable from a set of simultaneous equations. The network can now be solved for Z_{i 1}. Writing out the expression for input impedance gives;

$Z\_\{i\; 1\}\; =\; Z\; +\; frac\{1\}\{2Y+frac\{1\}\{Z+Z\_\{i\; 1\}$

and solving for Z_{i 1},

$Z\_\{i\; 1\}^2\; =\; Z^2\; +\; frac\{Z\}\{Y\}$

Z_{i 2} is found by a similar process, but it is simpler to work in terms of the reciprocal, that is image admittance Y_{i 2},

$Y\_\{i\; 2\}^2\; =\; Y^2\; +\; frac\{Y\}\{Z\}$

Also, it can be seen from these expressions that the two image impedances are related to each other by;

$frac\{Z\_\{i\; 1\{Y\_\{i\; 2\; =\; frac\{Z\}\{Y\}$

Useage in filter design

When used in filter design, the 'L' network analysed above is usually referred to as a half section. Two half sections in cascade will make either a T (tee) section or a Π (pi) section depending on which port of the L section comes first. This leads to the terminology of Z_{i T} to mean the Z_{i 1} in the above analysis and Z_{i Π} to mean Z_{i 2}.

Relation to characteristic impedance

Image impedance is a similar concept to the characteristic impedance used in the analysis of transmission lines. In fact, in the limiting case of a chain of cascaded networks where the size of each single network is approaching an infinitesimally small element, the mathematical limit of the image impedance expression is the characteristic impedance of the chain. That is,

$Z\_i^2\; ightarrow\; frac\{Z\}\{Y\}$

The connection between the two can further be seen by noting an alternative, but equivalent, definition of image impedance. In this definition, the image impedance of a network is the input impedance of an infinitely long chain of cascaded identical networks (with the ports arranged so that like impedance faces like). This is directly analogous to the definition of characteristic impedance as the input impedance of an infinitely long line.

Conversely, it is possible to analyse a transmission line with lumped components, such as one utilising loading coils, in terms of an image impedance filter.

Transfer function

The transfer function of the half section, like the image impedance, is calculated for a network terminated in its image impedances (or equivalently, as a section in an infinitely long chain of identical sections) and is given by,

$A(iomega)=sqrt\{frac\{Z\_\{I2\{Z\_\{I1\}e^\{-gamma\}$

where γ is called the transmission function, propagation function or transmission parameter and is given by,

$gamma=sinh^\{-1\}\{sqrt\{ZY$

The $sqrt\{frac\{Z\_\{I2\{Z\_\{I1\}$ term represents the voltage ratio that would be observed if the maximum available power was transferred from the source to the load. It would be possible to absorb this term into the definition of γ, and in some treatments this approach is taken. The purpose of separating it out is to scale γ so that $e^\{gamma\}$ has a magnitude of unity when maximum power is transferred, whatever the actual voltage ratio may be. In the case of a network with symmetrical image impedances, such as a chain of an even number of identical L sections, the expression reduces to,

$A(iomega)=e^\{-gamma\},!$

In general, γ is a complex number such that,

The real part of γ, represents an attenuation parameter, α in nepers and the imaginary part represents a phase change parameter, β in radians. The transmission parameters for a chain of n half sections, provided that like impedance always faces like, is given by;

$gamma\_n=ngamma,!$

As with the image impedance, the transmission parameters approach those of a transmission line as the filter section become infinitesimally small so that,

$gamma\; ightarrow\; sqrt\{ZY\}$

with α, β, γ, Z and Y all now being measured per metre instead of per half section.

ee also

* Constant k filters
* m-derived filters
* characteristic impedance

References

* Matthaei, Young, Jones "Microwave Filters, Impedance-Matching Networks, and Coupling Structures" McGraw-Hill 1964