models of two-port networks z, y, h, parameters

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  • 8/17/2019 Models of Two-port Networks Z, Y, H, parameters

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    Next: Active Circuits Up: Chapter 2: Circuit Principles Previous: NetworkTheorems

    Two-Port Networks

    Models of two-port networks

    Many complex passive and linear circuits can be modeled by a two-port networkmodel as shown below A two-port network is represented by !our external variables:

    volta"e and current at the input port# and volta"e and current at theoutput port# so that the two-port network can be treated as a black box modeled by the

    relationships between the !our variables # # and There exist six di!!erentways to describe the relationships between these variables# dependin" on which twoo! the !our variables are "iven# while the other two can always be derived

    • Z or impedance model: $iven two currents and !ind volta"es

    and by:

    http://fourier.eng.hmc.edu/e84/lectures/ch2/node5.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch2/node1.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch2/node3.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch2/node3.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch2/node1.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch2/node3.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch2/node3.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch2/node5.html

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    %ere all !our parameters # # # and represent impedance &n

    particular# and are transfer impedances # de!ined as the ratio o! a

    volta"e 'or ( in one part o! a network to a current 'or ( in another

    part is a 2 by 2 matrix containin" all !our parameters

    • Y or admittance model: $iven two volta"es and # !ind currents

    and by:

    %ere all !our parameters # # # and represent admittance &n

    particular# and are transfer admittances is the correspondin" parameter matrix

    • A or transmission model: $iven and # !ind and by:

    %ere and are dimensionless coe!!icients# is impedance and

    is admittance A ne"ative si"n is added to the output current in the model# sothat the direction o! the current is out-ward# !or easy analysis o! a cascade o!multiple network models

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    • H or !"rid model: $iven and # !ind and by:

    %ere and are dimensionless coe!!icients# is impedance andis admittance

    #enerali$ation to nonlinear circuits

    The two-port models can also be applied to a nonlinear circuit i! the variations o! thevariables are small and there!ore the nonlinear behavior o! the circuit can be piece-

    wise lineari)ed Assume is a nonlinear !unction o! variables and &!

    the variations and are small# the !unction can be approximated by a linearmodel

    with the linear coe!!icients

    %indin& t e model parameters

    *or each o! the !our types o! models# the !our parameters can be !ound !rom

    variables # # and o! a network by the !ollowin"

    • *or +-model:

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    • *or ,-model:

    *or A-model:

    • *or %-model:

    &! we !urther de!ine

    then the +-model and ,-model above can be written in matrix !orm:

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    'xample:

    *ind the +-model and ,-model o! the circuit shown

    • *irst assume # we "et

    • Next assume # we "et

    The parameters o! the ,-model can be !ound as the inverse o! :

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    Note:

    (om"inations of two-port models

    • eries connection o! two 2-port networks:

    • Parallel connection o! two 2-port networks:

    • Cascade connection o! two 2-port networks:

    'xample: A The circuit shown below contains a two-port network 'e " # a !ilter

    circuit# or an ampli!ication circuit( represented by a +-model:

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    The input volta"e is with an internal impedance and the load

    impedance is *ind the two volta"es # and two currents #

    Met od ):

    • *irst# accordin" the +-model# we have

    • econd# two more e.uations can be obtained !rom the circuit:

    • ubstitutin" the last two e.uations !or and into the !irst two# we "et

    • olvin" these we "et

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    • Then we can "et the volta"es

    Met od *: /e can also use Thevenin0s theorem to treat everythin" be!ore the load

    impedance as an e.uivalent volta"e source with Thevenin0s volta"e and

    resistance # and the output volta"e and current can be !ound

    • *ind with volta"e short-circuit:

    o The +-model:

    o Also due to the short-circuit o! volta"e source # we have

    o e.uatin" the two expressions !or # we "et

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    o ubstitutin" this into the e.uation !or above# we "et

    o *ind :

    • *ind open-circuit volta"e with :

    o ince the load is an open-circuit# # we have

    o *ind :

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    olvin" this to "et

    o *ind open-circuit volta"e :

    • *ind load volta"e :

    *ind load volta"e :

    Principle of reciprocit! :

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    Consider the example circuit on the le!t above# which can be simpli!ied as the network

    in the middle The volta"e source is in the branch on the le!t# while the current is inthe branch on the ri"ht# which can be !ound to be 'current divider(:

    /e next interchan"e the positions o! the volta"e source and the current# so that thevolta"e source is in the branch on the ri"ht and the current to be !ound is in the branchon the le!t# as shown on the ri"ht o! the !i"ure above The current can be !ound to be

    The two currents and are exactly the same1 This result illustrates the!ollowin" reciprocit! principle # which can be proven in "eneral:

    In any passive (without energy sources), linear network, if a voltage applied inbranch 1 causes a current in branch 2, then this voltage applied in branch 2

    will cause the same current in branch 1.This reciprocity principle can also be stated as:

    In any passive, linear network, the transfer impedance is equal to the reciprocal

    transfer impedance .

    ased on this reciprocity principle# any complex passive linear network can bemodeled by either a T-network or a -network:

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    • T-NetworkModel:

    *rom this T-model# we "et

    Comparin" this with the +-model# we "et

    olvin" these e.uations !or # and # we "et

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    • -NetworkModel:

    *rom this -model# we "et:

    Comparin" this with the ,-model# we "et

    olvin" these e.uations !or # and # we "et

    'xample ): Convert the "iven T-network to a network

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    +olution: $iven # # # we "et its +-model:

    The +-model can be expressed in matrix !orm:

    This +-model can be converted into a ,-model:

    This ,-model can be converted to a network:

    These admittances can be !urther converted into impedances:

    The same results can be obtained by , to delta conversion

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    'xample *: Consider the ideal trans!ormer shown in the !i"ure below

    Assume # # and the turn ratio is 3escribe thiscircuit as a two-port network

    • et up basic e.uations:

    • 4earran"e the e.uations in the !orm o! a +-model The second e.uation is

    ubstitutin" into the !irst e.uation# we "et

    The +-model is:

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    As # this is a reciprocal network

    Alternatively# we can set up the e.uations in terms o! the currents:

    • 4earran"e the e.uations in the !orm o! a ,-model The !irst e.uation is

    • ubstitutin" into the second e.uation# we "et

    The ,-model is:

    *inally# we can veri!y that

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    Next: Active Circuits Up: Chapter 2: Circuit Principles Previous: Network Theorems uye !ang 2"1#$"2$1%

    http://fourier.eng.hmc.edu/e84/lectures/ch2/node5.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch2/node1.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch2/node3.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch2/node5.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch2/node1.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch2/node3.html