Page 48 - Analog and Digital Filter Design
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                                                      Time and Frequency Response




                      output  signal  that  is  not  proportional  to the  frequency. The  rate  of  change
                      in phase with frequency is known as the group delay. The group delay increases
                      with the number of  filter stages, so a fourth-order filter will  produce a greater
                      delay than a third-order filter.

                      The group delay is the delay seen by all signal frequencies as they pass through
                      the filter. For example, a signal of  1 kHz may see a phase shift of  36", which is
                      a delay of 0.1 ms (the period of  a  1 kHz signal is  I ms and 36"  is 0.1 cycle). If
                      the phase change is proportional  to frequency, a 2 kHz signal will  see a phase
                      shift  of  72",  which  is  also  a  delay of  0.1 ms (the period  of  a  2 kHz  signal  is
                      0.5ms and  72"  is  0.2 cycle). This  represents  a  constant  group delay  because
                      both signals are delayed by the same amount.


                      An example of  a nonconstant group delay filter would be one where the  I kHz
                      signal is delayed by 0.1 ms, as before. Now suppose that the 2 kHz signal sees a
                      phase shift of 90", which is a delay of 0.125ms. The timing relationship between
                      the two signals has changed because the 2 kHz signal is delayed by 0.025 ms more
                      than the  1 kHz signal.

                      The consequence of  a  nonconstant  group delay can  be  seen when pulses are
                      applied to the filter input. Pulses contain signal harmonics several times the fun-
                      damental  frequency  of  the  pulse. As  these harmonics  propagate  through  the
                      filter, they each experience different delays. Summing the delayed fundamental
                      and harmonic signals results in slowly rising and falling pulse edges and causes
                      ripple on top of  the pulse. This distortion can produce errors when subsequent
                      circuits process the pulse.


                      Butterworth,  Chebyshev,  Inverse Chebyshev. and  Cauer  filters  have  a  group
                      delay that increases with frequency and reaches a peak value close to the cutoff
                      point. Beyond the cutoff point, the group delay gradually reduces to a constant
                      value. An example of  group delay for a third-order  Butterworth filter is given
                      in Figure 2.3.  The delay shown is for a filter having a  1 rad/s cutoff  frequency,
                      which is about 2 seconds at low frequencies. The delay is inversely proportional
                      to the cutoff frequency, so a filter having a  1 kHz (6283 rad/s) cutoff frequency
                      will  have a delay of  2/6283, or 3 I8 ps, at low frequencies.


                      Further information on group delay is provided in Chapter 9, which describes
                      all-pass filters. All-pass filters have a phase response that can be used to correct
                      group delay variations of  band-shaping filters. All-pass filters can also be used
                      to create Hilbert transform filters. These have two filter branches whose outputs
                      have the same signal amplitude but  with a 90" phase difference. Hilbert filters
                      are used to create single-sideband modulation of  a radio carrier signal.
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