Page 346 - Fundamentals of Radar Signal Processing
P. 346

(5.20)

               where k absorbs constants resulting from the matrix inversion.
                     S  represents the available information on the interference. The elements on
                       I
               the main diagonal will always be identical and equal to the total interference
               power, which is the sum of the independent interference source powers. The
               off-diagonal  elements  represent  the  correlation  properties  of  the  interference
               over  one  PRI.  Because  the  noise  is  white,  it  does  not  contribute  to  the  off-
               diagonal elements, whereas the clutter does contribute provided ρ = ρ [1] ≠ 0.
                                                                                                    c
               More  generally,  an Nth order filter will require the N × N covariance matrix
               and will involve correlation coefficients up to ρ [N – 1].
                                                                        c
                     To  finish  computing h,  a  model  is  needed  for  the  assumed  target  signal
               phase history t. For a target moving at a constant radial velocity, the expected
               target  signal  is  just  a  discrete  complex  sinusoid  at  the  appropriate  Doppler
               frequency F . Following the discussion in Sec. 2.6.3, assume the waveform is a
                             D
               train of M simple pulses with PRI T and RF transmit frequency F. If the target is
                                                                                            t
               at a nominal range R  and is moving toward the radar at a radial velocity of v
                                        0
               meters per second, the slow-time phase history will be of the form








                                                                                                       (5.21)

               where F  = 2v/λ is the usual Doppler shift, R  ≈ R  is the range corresponding to
                                                                    s
                         D
                                                                          0
               the sampling time, and all constants are absorbed into A at each step.
                     Only N samples at a time of y[m] are of interest in analyzing an N-sample
               canceller.  Assuming N  ≤ M  and  recalling  the  results  of App.  B  on  vector
               representation  of  linear  filtering,  the  series  of N  samples  ending  at m  = m ,
                                                                                                            0
               {y[m ], y[m  – 1], …, y[m  – N + 1]}, can be represented in vector form as
                                              0
                             0
                     0





                                                                                                       (5.22)

               where the phase terms due to the delay to the first sample of interest, m , have
                                                                                                      0
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