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Impedance parameters
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<h2 id="the-z-parameter-matrix">The Z-parameter matrix</h2> <p>A Z-parameter matrix describes the behaviour of any linear electrical network that can be regarded as a <a href="/facts/Black_box/hJeAGnIz">black box</a> with a number of <a href="/facts/Port_(circuit_theory)/g2mokqv0">ports</a>. A <i>port</i> in this context is a pair of <a href="/facts/Terminal_(electronics)/CwbKGSuB">electrical terminals</a> carrying equal and opposite currents into and out-of the network, and having a particular <a href="/facts/Voltage/EN2po6N2">voltage</a> between them. The Z-matrix gives no information about the behaviour of the network when the currents at any port are not balanced in this way (should this be possible), nor does it give any information about the voltage between terminals not belonging to the same port. Typically, it is intended that each external connection to the network is between the terminals of just one port, so that these limitations are appropriate. </p><p>For a generic multi-port network definition, it is assumed that each of the ports is allocated an integer <i>n</i> ranging from 1 to <i>N</i>, where <i>N</i> is the total number of ports. For port <i>n</i>, the associated Z-parameter definition is in terms of the port current and port voltage, I n {\displaystyle I_{n}\,} and V n {\displaystyle V_{n}\,} respectively. </p><p>For all ports the voltages may be defined in terms of the Z-parameter matrix and the currents by the following matrix equation: </p> V = Z I {\displaystyle V=ZI\,} <p>where Z is an <i>N</i> × <i>N</i> matrix the elements of which can be indexed using conventional <a href="/facts/Matrix_(mathematics)/qa8FI4ko">matrix</a> notation. In general the elements of the Z-parameter matrix are <a href="/facts/Complex_number/2w7mqI7e">complex numbers</a> and functions of frequency. For a one-port network, the Z-matrix reduces to a single element, being the ordinary <a href="/facts/Electrical_impedance/I06NSXtN">impedance</a> measured between the two terminals. The Z-parameters are also known as the open circuit parameters because they are measured or calculated by applying current to one port and determining the resulting voltages at all the ports while the undriven ports are terminated into open circuits. </p> <h2 id="two-port-networks">Two-port networks</h2> <p>The Z-parameter matrix for the <a href="/facts/Two-port_network/cqUrBTYq">two-port network</a> is probably the most common. In this case the relationship between the port currents, port voltages and the Z-parameter matrix is given by: </p> ( V 1 V 2 ) = ( Z 11 Z 12 Z 21 Z 22 ) ( I 1 I 2 ) {\displaystyle {\begin{pmatrix}V_{1}\\V_{2}\end{pmatrix}}={\begin{pmatrix}Z_{11}&Z_{12}\\Z_{21}&Z_{22}\end{pmatrix}}{\begin{pmatrix}I_{1}\\I_{2}\end{pmatrix}}} . <p>where </p> Z 11 = V 1 I 1 | I 2 = 0 Z 12 = V 1 I 2 | I 1 = 0 {\displaystyle Z_{11}={V_{1} \over I_{1}}{\bigg |}_{I_{2}=0}\qquad Z_{12}={V_{1} \over I_{2}}{\bigg |}_{I_{1}=0}} Z 21 = V 2 I 1 | I 2 = 0 Z 22 = V 2 I 2 | I 1 = 0 {\displaystyle Z_{21}={V_{2} \over I_{1}}{\bigg |}_{I_{2}=0}\qquad Z_{22}={V_{2} \over I_{2}}{\bigg |}_{I_{1}=0}} <p>For the general case of an <i>N</i>-port network, </p> Z n m = V n I m | I k = 0 for k ≠ m {\displaystyle Z_{nm}={V_{n} \over I_{m}}{\bigg |}_{I_{k}=0{\text{ for }}k\neq m}} <h3>Impedance relations</h3> <p>The input impedance of a two-port network is given by: </p> Z in = Z 11 − Z 12 Z 21 Z 22 + Z L {\displaystyle Z_{\text{in}}=Z_{11}-{\frac {Z_{12}Z_{21}}{Z_{22}+Z_{L}}}} <p>where ZL is the impedance of the load connected to port two. </p><p>Similarly, the output impedance is given by: </p> Z out = Z 22 − Z 12 Z 21 Z 11 + Z S {\displaystyle Z_{\text{out}}=Z_{22}-{\frac {Z_{12}Z_{21}}{Z_{11}+Z_{S}}}} <p>where ZS is the impedance of the source connected to port one. </p> <h2 id="relation-to-s-parameters">Relation to S-parameters</h2> <p>The Z-parameters of a network are related to its <a href="/facts/S-parameters/z6ffeKh6">S-parameters</a> by<a class="footnote-ref" id="fnref:5" href="#fn:5"><sup>5</sup></a> </p> Z = z ( 1 N + S ) ( 1 N − S ) − 1 z = z ( 1 N − S ) − 1 ( 1 N + S ) z {\displaystyle {\begin{aligned}Z&={\sqrt {z}}(1_{\!N}+S)(1_{\!N}-S)^{-1}{\sqrt {z}}\\&={\sqrt {z}}(1_{\!N}-S)^{-1}(1_{\!N}+S){\sqrt {z}}\\\end{aligned}}} <p>and<a class="footnote-ref" id="fnref:6" href="#fn:6"><sup>6</sup></a> </p> S = ( y Z y − 1 N ) ( y Z y + 1 N ) − 1 = ( y Z y + 1 N ) − 1 ( y Z y − 1 N ) {\displaystyle {\begin{aligned}S&=({\sqrt {y}}Z{\sqrt {y}}\,-1_{\!N})({\sqrt {y}}Z{\sqrt {y}}\,+1_{\!N})^{-1}\\&=({\sqrt {y}}Z{\sqrt {y}}\,+1_{\!N})^{-1}({\sqrt {y}}Z{\sqrt {y}}\,-1_{\!N})\\\end{aligned}}} <p>where 1 N {\displaystyle 1_{\!N}} is the <a href="/facts/Identity_matrix/Glbcf6ol">identity matrix</a>, z {\displaystyle {\sqrt {z}}} is a <a href="/facts/Diagonal_matrix/tjIAHrE6">diagonal matrix</a> having the square root of the <a href="/facts/Characteristic_impedance/oUg0mhah">characteristic impedance</a> at each port as its non-zero elements, </p><p> z = ( z 01 z 02 ⋱ z 0 N ) {\displaystyle {\sqrt {z}}={\begin{pmatrix}{\sqrt {z_{01}}}&\\&{\sqrt {z_{02}}}\\&&\ddots \\&&&{\sqrt {z_{0N}}}\end{pmatrix}}} </p><p>and y = ( z ) − 1 {\displaystyle {\sqrt {y}}=({\sqrt {z}})^{-1}} is the corresponding diagonal matrix of square roots of <a href="/facts/Characteristic_admittance/tG383LcM">characteristic admittances</a>. In these expressions the matrices represented by the bracketed factors <a href="/facts/Commuting_matrices/R1wGesmf">commute</a> and so, as shown above, may be written in either order.<a class="footnote-ref" id="fnref:7" href="#fn:7"><sup>7</sup></a><a class="footnote-ref" id="fnref:8" href="#fn:8"><sup>8</sup></a> </p> <h3>Two port</h3> <p>In the special case of a two-port network, with the same characteristic impedance z 01 = z 02 = Z 0 {\displaystyle z_{01}=z_{02}=Z_{0}} at each port, the above expressions reduce to </p> Z 11 = ( ( 1 + S 11 ) ( 1 − S 22 ) + S 12 S 21 ) Δ S Z 0 {\displaystyle Z_{11}={((1+S_{11})(1-S_{22})+S_{12}S_{21}) \over \Delta _{S}}Z_{0}\,} Z 12 = 2 S 12 Δ S Z 0 {\displaystyle Z_{12}={2S_{12} \over \Delta _{S}}Z_{0}\,} Z 21 = 2 S 21 Δ S Z 0 {\displaystyle Z_{21}={2S_{21} \over \Delta _{S}}Z_{0}\,} Z 22 = ( ( 1 − S 11 ) ( 1 + S 22 ) + S 12 S 21 ) Δ S Z 0 {\displaystyle Z_{22}={((1-S_{11})(1+S_{22})+S_{12}S_{21}) \over \Delta _{S}}Z_{0}\,} <p>Where </p> Δ S = ( 1 − S 11 ) ( 1 − S 22 ) − S 12 S 21 {\displaystyle \Delta _{S}=(1-S_{11})(1-S_{22})-S_{12}S_{21}\,} <p>The two-port S-parameters may be obtained from the equivalent two-port Z-parameters by means of the following expressions<a class="footnote-ref" id="fnref:9" href="#fn:9"><sup>9</sup></a> </p> S 11 = ( Z 11 − Z 0 ) ( Z 22 + Z 0 ) − Z 12 Z 21 Δ {\displaystyle S_{11}={(Z_{11}-Z_{0})(Z_{22}+Z_{0})-Z_{12}Z_{21} \over \Delta }} S 12 = 2 Z 0 Z 12 Δ {\displaystyle S_{12}={2Z_{0}Z_{12} \over \Delta }\,} S 21 = 2 Z 0 Z 21 Δ {\displaystyle S_{21}={2Z_{0}Z_{21} \over \Delta }\,} S 22 = ( Z 11 + Z 0 ) ( Z 22 − Z 0 ) − Z 12 Z 21 Δ {\displaystyle S_{22}={(Z_{11}+Z_{0})(Z_{22}-Z_{0})-Z_{12}Z_{21} \over \Delta }} <p>where </p> Δ = ( Z 11 + Z 0 ) ( Z 22 + Z 0 ) − Z 12 Z 21 {\displaystyle \Delta =(Z_{11}+Z_{0})(Z_{22}+Z_{0})-Z_{12}Z_{21}\,} <p>The above expressions will generally use complex numbers for S i j {\displaystyle S_{ij}\,} and Z i j {\displaystyle Z_{ij}\,} . Note that the value of Δ {\displaystyle \Delta \,} can become 0 for specific values of Z i j {\displaystyle Z_{ij}\,} so the division by Δ {\displaystyle \Delta \,} in the calculations of S i j {\displaystyle S_{ij}\,} may lead to a division by 0. </p> <h2 id="relation-to-y-parameters">Relation to Y-parameters</h2> <p>Conversion from <a href="/facts/Y-parameters/0PJ6u6IH">Y-parameters</a> to Z-parameters is much simpler, as the Z-parameter matrix is just the <a href="/facts/Matrix_inverse/fPqXk3V8">inverse</a> of the Y-parameter matrix. For a two-port: </p> Z 11 = Y 22 Δ Y {\displaystyle Z_{11}={Y_{22} \over \Delta _{Y}}\,} Z 12 = − Y 12 Δ Y {\displaystyle Z_{12}={-Y_{12} \over \Delta _{Y}}\,} Z 21 = − Y 21 Δ Y {\displaystyle Z_{21}={-Y_{21} \over \Delta _{Y}}\,} Z 22 = Y 11 Δ Y {\displaystyle Z_{22}={Y_{11} \over \Delta _{Y}}\,} <p>where </p> Δ Y = Y 11 Y 22 − Y 12 Y 21 {\displaystyle \Delta _{Y}=Y_{11}Y_{22}-Y_{12}Y_{21}\,} <p>is the <a href="/facts/Determinant/eGYqJ2TF">determinant</a> of the Y-parameter matrix. </p> <h2 id="notes">Notes</h2> <h2 id="bibliography">Bibliography</h2> <ul><li>David M. Pozar (2004-02-05). <i>Microwave Engineering</i>. Wiley. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-471-44878-5.</li> <li>Simon Ramo; John R. Whinnery; Theodore Van Duzer (1994-02-09). <i>Fields and Waves in Communication Electronics</i>. Wiley. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-471-58551-0.</li></ul> <h2 id="see-also">See also</h2> <ul><li><a href="/facts/Scattering_parameters/z6ffeKh6">Scattering parameters</a></li> <li><a href="/facts/Admittance_parameters/0PJ6u6IH">Admittance parameters</a></li> <li><a href="/facts/Two-port_network/cqUrBTYq">Two-port network</a></li></ul> <h2 id="references">References</h2> <ol> <li id="fn:1"><p>David M. Pozar (2004-02-05). Microwave Engineering. Wiley. pp. 170–174. ISBN 978-0-471-44878-5. <a href="978-0-471-44878-5" target="_blank">978-0-471-44878-5</a> <a href="#fnref:1" class="footnote-back-ref">↩</a></p></li> <li id="fn:2"><p>David M. Pozar, 2005 (op. cit); pp 170-174. <a href="#fnref:2" class="footnote-back-ref">↩</a></p></li> <li id="fn:3"><p>David M. Pozar, 2005 (op. cit); pp 183-186. <a href="#fnref:3" class="footnote-back-ref">↩</a></p></li> <li id="fn:4"><p>A.H. Morton, Advanced Electrical Engineering, Pitman Publishing Ltd., 1985; pp 33-72, ISBN 0-273-40172-6. <a href="/wiki/ISBN_(identifier)" target="_blank">/wiki/ISBN_(identifier)</a> <a href="#fnref:4" class="footnote-back-ref">↩</a></p></li> <li id="fn:5"><p>Russer, Peter (2003). Electromagnetics, microwave circuit and antenna design for communications engineering. Artech House. p. 420. ISBN 1-58053-532-1. <a href="1-58053-532-1" target="_blank">1-58053-532-1</a> <a href="#fnref:5" class="footnote-back-ref">↩</a></p></li> <li id="fn:6"><p>Russer, Peter (2003). Electromagnetics, microwave circuit and antenna design for communications engineering. Artech House. p. 420. ISBN 1-58053-532-1. <a href="1-58053-532-1" target="_blank">1-58053-532-1</a> <a href="#fnref:6" class="footnote-back-ref">↩</a></p></li> <li id="fn:7"><p>Russer, Peter (2003). Electromagnetics, microwave circuit and antenna design for communications engineering. Artech House. p. 420. ISBN 1-58053-532-1. <a href="1-58053-532-1" target="_blank">1-58053-532-1</a> <a href="#fnref:7" class="footnote-back-ref">↩</a></p></li> <li id="fn:8"><p>Any square matrix commutes with itself and with the identity matrix, and if two matrices A and B commute, then so do A and B−1 (since AB−1 = B−1BAB−1 = B−1ABB−1 = B−1A) <a href="#fnref:8" class="footnote-back-ref">↩</a></p></li> <li id="fn:9"><p>Simon Ramo; John R. Whinnery; Theodore Van Duzer (1994-02-09). Fields and Waves in Communication Electronics. Wiley. pp. 537–541. ISBN 978-0-471-58551-0. <a href="978-0-471-58551-0" target="_blank">978-0-471-58551-0</a> <a href="#fnref:9" class="footnote-back-ref">↩</a></p></li> </ol>