z parameters / Impedance Parameters / open circuit parameters in two port network

After reading this z parameter in two port network, you will understand the theory, how to determine z parameters, the condition of symmetry & reciprocity and applications.


General theory of z parameters

In two port network, the terminal input and output voltages V1 and V2 can be expressed in terms of the terminal input and output currents I1 and I2.

z parameters

As shown in Figure 1, the terminal voltages can be written in terms of the terminal currents as

${{\mathbf{V}}_1} = {{\mathbf{z}}_{{\text{11}}}}{{\mathbf{I}}_1} + {{\mathbf{z}}_{{\text{12}}}}{{\mathbf{I}}_2}$   …..(1)

${{\mathbf{V}}_2} = {{\mathbf{z}}_{{\text{21}}}}{{\mathbf{I}}_1} + {{\mathbf{z}}_{{\text{22}}}}{{\mathbf{I}}_2}$   …..(2)

From Eq.(1) and Eq.(2), it can be concluded that the terminal voltages are dependent variables and the terminal currents are independent variables. Also, using Eq.(1) and Eq.(2), the equivalent circuit represented as shown in Figure 2.

 

z parameters

By using Eq.(1) and Eq.(2), can be written in matrix form as

$\left[ {\begin{array}{*{20}{c}}
{{{\mathbf{V}}_1}} \\
{{{\mathbf{V}}_2}}
\end{array}} \right] = \left[ {\begin{array}{*{20}{c}}
{{{\mathbf{z}}_{{\text{11}}}}}&{{{\mathbf{z}}_{{\text{12}}}}} \\
{{{\mathbf{z}}_{{\text{21}}}}}&{{{\mathbf{z}}_{{\text{22}}}}}
\end{array}} \right]\left[ {\begin{array}{*{20}{c}}
{{{\mathbf{I}}_1}} \\
{{{\mathbf{I}}_2}}
\end{array}} \right]$

The above matrix can be generalized as

$\left[ {\mathbf{V}} \right] = \left[ {\mathbf{z}} \right]\left[ {\mathbf{I}} \right]$

where [z] matrix,

$\left[ {\mathbf{z}} \right] = \left[ {\begin{array}{*{20}{c}}
{{{\mathbf{z}}_{{\text{11}}}}}&{{{\mathbf{z}}_{{\text{12}}}}} \\
{{{\mathbf{z}}_{{\text{21}}}}}&{{{\mathbf{z}}_{{\text{22}}}}}
\end{array}} \right]$

The elements of matrix [z] are called z parameters and each parameters having unit in ohm.

How to determine z parameters?

  • The z parameters, z11 and z21 are obtained by open circuiting the port 2 i.e. I2 = 0 along with connecting voltage source V1 to port 1 as shown in Figure 3. Thus we get

\[{{\mathbf{z}}_{{\text{11}}}} = {\left. {\frac{{{{\mathbf{V}}_1}}}{{{{\mathbf{I}}_1}}}} \right|_{{{\mathbf{I}}_2} = 0}}\]

${{\mathbf{z}}_{{\text{11}}}}{\text{ is Open – circuit driving point input impedance}}{\text{.}}$

\[{{\mathbf{z}}_{{\text{21}}}} = {\left. {\frac{{{{\mathbf{V}}_2}}}{{{{\mathbf{I}}_1}}}} \right|_{{{\mathbf{I}}_2} = 0}}\]

${{\mathbf{z}}_{{\text{21}}}}{\text{ is Open – circuit forward transfer impedance }}{\text{.}}$

z parameters

  • The z parameters, z22 and z12 are obtained by open circuiting the port 1 i.e. I1 = 0 along with connecting voltage source V2 to port 2 as shown in Figure 4. Thus we get

\[{{\mathbf{z}}_{{\text{12}}}} = {\left. {\frac{{{{\mathbf{V}}_1}}}{{{{\mathbf{I}}_2}}}} \right|_{{{\mathbf{I}}_1} = 0}}\]

\[{{\mathbf{z}}_{{\text{12}}}}{\text{ is Open – circuit reverse transfer impedance}}{\text{.}}\]

\[{{\mathbf{z}}_{22}} = {\left. {\frac{{{{\mathbf{V}}_2}}}{{{{\mathbf{I}}_2}}}} \right|_{{{\mathbf{I}}_1} = 0}}\]

${{\mathbf{z}}_{22}}{\text{ is Open – circuit driving point output impedance}}{\text{.}}$

Note:- For z parameters, the terminal voltage V1 and V2 are function of terminal currents I1 and I2 as

\[\left( {{{\mathbf{V}}_1},{{\mathbf{V}}_2}} \right) = {\text{f }}\left( {{{\mathbf{I}}_1},{{\mathbf{I}}_2}} \right)\]

z parameters

Condition of symmetry

A two port network is said to be symmetrical if the ratio of response to excitation remains same at both ports independently with respect to the defined circuit conditions such as open circuit or short circuit. Thus, we can say

\[{\left. {\frac{{{{\mathbf{V}}_1}}}{{{{\mathbf{I}}_1}}}} \right|_{{{\mathbf{I}}_2} = 0}} = {\left. {\frac{{{{\mathbf{V}}_2}}}{{{{\mathbf{I}}_2}}}} \right|_{{{\mathbf{I}}_1} = 0}}\]

\[{\text{or, }}{{\mathbf{z}}_{11}} = {{\mathbf{z}}_{22}}\]

Condition of reciprocity

A two port network is said to be reciprocal if the ratio of response to excitation remains same even when the position of response to excitation are interchanged. Thus, we can say

\[{\left. {\frac{{{{\mathbf{V}}_1}}}{{{{\mathbf{I}}_2}}}} \right|_{{{\mathbf{I}}_1} = 0}} = {\left. {\frac{{{{\mathbf{V}}_2}}}{{{{\mathbf{I}}_1}}}} \right|_{{{\mathbf{I}}_2} = 0}}\]

\[{\text{or, }}{{\mathbf{z}}_{12}} = {{\mathbf{z}}_{21}}\]

Applications

  • Use for filters Combination.
  • design of impedance-matching networks
  • design of power distribution networks.

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