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4.11 Reference Filters                                               139


        for the filter in Figure 4.19. The filter is a fifth-order LC ladder structure with
        Chebyshev I characteristic.
            Figure 4.18 also shows the
        variations in the attenuation for
        very large changes (±20% from the
        nominal value) of one of the induc-
        tances in the ladder structure. The
        passband ripple has been chosen to
        be a very large value, A max = 3 dB,
        in order to demonstrate the low    Figure 4.18 Double resistively terminated
        sensitivity.                                 reactance network
            A counterintuitive property of
        these filters is that sensitivity in
        the passband is reduced if the rip-
        ple is reduced. It follows from Fett-
        weis-Orchard's argument that the
        attenuation is bounded from below
        (the magnitude function is bounded
        from above) by the maximum power
        transfer constraint. This lower
        value is usually normalized to 0 dB.
        Hence, if any element value in the
        lossless network deviates from its  Figure 4.19 Attenuation in the passband for a
        nominal value, the attenuation               fifth-order LC filter with nominal
        must necessarily increase and can-           element values and ±20%
                                                     deviation in one of the inductors
        not decrease independently of the
        sign of the deviation. Thus, for these
        frequencies the sensitivity is zero, i.e.,




        where e represents any element in the lossless network—for example, an induc-
        tance. These filters are optimal for frequency-selective filters with "flat" pass-
        bands. The sensitivity in the stopband depends on the internal structure of the
        reactance network. Usually, lattice or ladder networks are used.
            Many schemes for simulating doubly terminated LC networks have been
        developed for active RC filters [24]. Unfortunately, the problem of simulating an
        analog reference filter using a digital network is a nontrivial problem. Generally, a
        nonsequentially computable algorithm is obtained (see Chapter 6). However,
        Alfred Fettweis [7—10] has developed a comprehensive theory, the wave digital fil-
        ter theory, which solves the problem. Indeed, it is not only a theory for design of
        digital filters, it is also a general theory describing the relationships between cer-
        tain discrete-time networks and certain classes of lumped and distributed element
                                                                   2
        networks. Furthermore, it inherently contains an energy concept  which can be
        used to guarantee stability in nonlinear digital networks.



        2
        - There exists a Lyanuponov function for wave digital filter structures.
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