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Bandstop Filters  22 1





                            J = zero frequency.

                                 fR2R
                            R6=-      when  fR >.fx or when fR  < f-.
                                  fz
                      R6 = R when an all-pole filter is required, since fR = f- and R5 is not connected
                      (see the State Variable Bandstop Filters section).

                      The resistors labeled R and R’ can be any arbitrary value; a typical value may
                      be in the range 1 kQ to 100 kQ; say 10 kQ. The resistors labeled R have an effect
                      on the input impedance of  the filter section. The value of  R should be several
                      times higher than the input signal’s source impedance.



                Denormalization oi Bandstop Biquad Filter Section

                      Consider a hypothetical design for a Cauer filter section that will produce a pole
                      and a zero. This design has a pole  fR = 280rad/s, which has Q = 15. The zero for
                      this design will be at 300radk

                            Let C=O.l,uFandletR=R’= 10kQ.












                            R6=-=8711Q.
                                 fR2
                                  fi

                Reference

                      i.    Williams, A., and E J. Taylor. Electronic  Filter. Des@  Handbook. New
                            York: McGraw-Hill, 1988.

                Exercises


                      7. I   Describe the step-by-step process for designing a passive bandstop
                            filter, starting with a lowpass prototype.
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