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and using Equation (15-8), then



                                      VщlJt) =  [У р siп(Э)]  Х P(t)

            which agrees with  Figures 15-7, 15-9, and  15-11 for е =  О, 90,  and 270 degrees.

            Now  let's take  а look at а situation  where  the  input signal's frequency  f;o_h;  is  just
            above  the  sampling  frequency  (Figure  15-12).  This  figure  shows  ап input signal
            whose  frequency  is  slightly  above  the  sampling  frequency  that  is  sampled  at
            various  amplitude  ranges of the input signal,  which  provides  а varying  signal  at the
            output  of the  sampling  system  (Figure  15-13).  This  figure  shows  the  result  of

            sampling  ап input  signal  whose frequency  f;o  h;  is  slightly  higher than  the sampling
            frequency  f .  Note  that the  input signal's peak  sinusoidal  amplitude  is  one-half the
                         s
            amplitude of the pulse-train signal.  Notice that the  resulting  signal  from  the output
            of the  sampleг looks like  а low-fгequency signal  at  (f;n_h; - f ),  and  it has  the  same
                                                                                  s
            amplitude as  the input signal  that is  being  sampled  ог multiplied  Ьу the pulse-train
            signal  (Figures 15-14 and  15-15).
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