Page 268 - Analog and Digital Filter Design
P. 268

Phase-Shift Networks (All-Pass Filters)  265






                  rp =  1.0;
                  ip =  0~0;
                  for(k =  1:  k  c= order;  ktt)
                         1
                         x =  (2*k -  l)*Pi/(2.0*order);
                         1  =  0.5  *  (gamma +  l.O/gamma)   cos(x);
                         r  =  -0.5  *  (gama - l.O.'gamma)  *  sin(x);
                         rpt =  ip*(i-normalizedfrequencyl - rp*r;
                         ipt =  rp*(normalizedFrequency-il - r*ip;
                         ip =  ipt;
                         rp =  rpt;
                         I
                  *magnitude =  20.0  *  loglO(hSubZero:sqrtlip*ip +  rp*rp) 1:
                  *phase =  180.0  *  atan2:  ip,  rpl  /PI;
                  recur3 ;
                  1
                  Listing 9.1
                  Subroutine "chebyshevFreqResonse( 1''




                  Equalizer equations given in the same MATHCAD application were then used
                  to find the minimum group delay variation. The coefficients for the equations
                  were adjusted until the sum of equalizer and filter group delay variations were
                  minimized. This was  carried  out  by  eye,  rather  than  using  an  optimization
                  routine. The lowest  variation in  group delay occurred when the group delay
                  was equi-ripple; that is, the peaks all had the same amplitude and the troughs
                  all had the same amplitude. The resulting equalization pole factors, such as mR
                  and Q, have been calculated for Chebyshev filters with 0.01 dB, 0.1 dB, 0.25d3,
                  0.5dB,  and  1dB passband ripple. As in the Butterworth design case, higher-
                  order filters are more difficult to equalize. This also applies as the passband
                  ripple increases: 0.01dB  ripple filters are easier to  equalize than  IdB-ripple
                  designs.

                  The calculated pole factors for Chebyshev filter equalizers are given in Tables
                  9.4 to  9.8. The number of  designs equalized was limited to filter-orders that
                  gave practical results. It was not sensible to equalize filters where the equalizer
                  would be far more complicated than the filter itself. Passive equalizer compo-
                  nent values have been calculated for several Chebyshev filter designs from the
                  equalization pole factors. using the equations given earlier in this chapter. Again.
                  component values to equalize Chebyshev filters with 0.01 dB, 0. I dB, 0.25dB.
                  0,5dB, and  1dB passband  ripple  were  calculated. Component  values  for  a
                  limited number of  practical passive equalizers are given in Tables 9.9 to 9.13.
                  Active equalizer values are not given because these depend on some user-defined
                  variables.
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