Page 408 - Analog and Digital Filter Design
P. 408

IIR Filter Design   405




                      The firsl term in the denominator is required to be  1.0 instead of  24.2403455,
                      so all terms in the equation must be divided by 24.2403455. The Al term in the
                      numerator for the biquad is positive, so the coefficient A 1 will be negative. Also
                      the Bl and B2 terms in the denominator should both be negative. so coefkients
                      BI  and B2 have negative values. Carrying out these changes gives:

                                  0.041253537 + (-0.082507074). Z-'  + 0.041253537.~-~
                            H(z) =
                                        1 - (-1.348967736)  - (-0.51 3981886. z-!)

                      Now  this  means  that  the  coefficient  values  are  A0  =  0.041253537,  A1  =
                     -0.082507074,  A2 = 0.041253537, B1 = -1.348967736,  and B2 = -0.513981885.
                      This completes the design process using method  1 ~



                      Design Method 2
                      In the second highpass filter method, s is replaced by:
                            s = tan(wD/2). [;y

                                         -

                      Now by substituting into the original Butterworth transfer function


                                       1
                            N(s) =
                                  S'+&S+l
                      Using mD = 2rr(3.4/8) = 2.670353756, the function tan(mD/2) = tan(1.335176878)
                      = 4.165299774. It is now possible to substitute for s:




                                                      1
                            H(z) =
                                                +I
                                                     +
                                  17.3497222 1. [3] 5.890623432. [+]  + 1
                                               7-                  Z-1
                      By comparing design method 1 and 2, it can be seen that the results using design
                      method 2 are identical (within calculator error limits). The only difference is that
                      the second method is a single step.



                      Bandpass Frequency Scaling
                      Bandpass frequency  scaling is more complex than either Iowpass or highpass
                      transformation and scaling. Lowpass to bandpass transformation and frequency
   403   404   405   406   407   408   409   410   411   412   413