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4.13 Transmission Lines                                              141

        tures can be mapped to classical filter structures with lumped circuit elements and
        we can make full use of the abundant knowledge of lumped element niters.




        4.13 TRANSMISSION LINES

        A special case of filter networks with distributed circuit elements is commensurate-
        length transmission line filters in which all lines have a common electrical propa-
        gation time. A lossless transmission line can be described as a two-port by the
        chain matrix










        where ZQ is the characteristic imped-
        ance and T/2 is the propagation time in
        each direction as illustrated in Figure
        4.21. ZQ is a real positive constant cure
        (Zo = R) for lossless transmission lines
        and is therefore sometimes called the
        characteristic resistance, while lossless
        transmission lines are often referred to
        as unit elements. Obviously, a transmis-  Figure 4.21 Transmission line
        sion line cannot be described by poles
        and zeros since the elements in the
        chain matrix are not rational functions
        ins.
           Wave digital filters imitate reference filters built out of resistors and lossless
        transmission lines by means of incident and reflected voltage waves. Computable
        digital filter algorithms can be obtained if the reference filter is designed using
        only such transmission lines. Wave digital filter design involves synthesis of such
        reference filters.
           Commensurate-length transmission line filters constitute a special case of dis-
        tributed element networks that can easily be designed by mapping them to a
        lumped element structure. This mapping involves Richards' variable which is
        defined as





        where f= £ +jQ. Richards' variable is a dimensionless complex variable. The real
        frequencies in the s- and f-domains are related by
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