Page 375 - Fundamentals of Radar Signal Processing
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multiplying  the  data  by  a  truncated,  asymmetric  window  (the  portion  of  the

               actual  window  that  overlaps  the M  nonzero  data  points),  resulting  in  greatly
               increased  sidelobes.  Applying  a  shortened K-point  window  to  a  turned  data
               sequence results in DFT samples that do not equal samples of the DTFT of the
               windowed M-point original data sequence.
                     Because the DFT is a sampled version of the DTFT, the peak value of the
               DFT  obtained  for  a  pure  sinusoidal  signal  is  greatest  when  the  Doppler

               frequency  coincides  exactly  with  one  of  the  DFT  sample  frequencies,  and
               decreases when the target signal is between DFT frequencies. This reduction in
               amplitude is called a Doppler straddle loss. The amount of loss depends on the
               particular  window  used  and  the  ratio K/M.  For  a  given  signal  length M,  the
               straddle loss is always greatest for signal frequencies exactly halfway between
               DFT sample frequencies. The calculation can be simplified by assuming that the
               signal frequency is F  = 0 so that y[m] = w[m] and then evaluating Eq. (5.81)
                                        D
               with k = 0 (DFT sample on the “sinusoid” peak) and k = 1/2 (1/2 bin away from
               the sinusoid peak). To be explicit, consider the rectangular window case; then







                                                                                                       (5.82)

               Assuming K ≥ M and evaluating at k = 1/2 gives






                                                                                                       (5.83)


               The last step was obtained by assuming that K is large enough to allow a small
               angle  approximation  to  the  sine  function  in  the  denominator. Y[0] is obtained
               either  by  applying  L’HÔpital’s  rule  to  the  second  form  of Eq.  (5.82)  or
               computing it explicitly from the first form; the result is Y [0] = M. The maximum
               straddle loss for the DFT filterbank with no windowing is






                                                                                                       (5.84)

               This equation verifies that the loss depends on the ratio K/M. The worst case

               occurs when the sinc term is minimized; this happens when K = M. In decibels,
               this worst-case loss for a rectangular window is sinc (1/2) = sin(π/2)/(π/2) =
               2/π, equivalent to –3.92 dB.
                     The straddle loss for shaped windows varies somewhat with M as can be
               seen  in Table  5.2.  A  calculation  for  the  Hamming  window  similar  to  that
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