Page 154 - Fundamentals of Radar Signal Processing
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(2.102)


               Equation (2.102) shows that the range is approximately a quadratic function of

               time for the crossing target scenario of Fig. 2.25. Using this truncated series in
               Eq. (2.98) gives







                                                                                                     (2.103)

               All  of  the  terms  are  the  same  as  in  the  constant-velocity  case  of Eq.  (2.99)
               except  for  the  middle  exponential.  Recall  that  instantaneous  frequency  is
               proportional  to  the  time  derivative  of  phase.  The  quadratic  phase  function
               therefore represents a Doppler frequency shift that varies linearly with time due
               to the changing radar-target geometry:







                                                                                                     (2.104)

                     As  the  target  aircraft  approaches  from  the  left  in Fig.  2.25  (t  <  0)  the

               instantaneous Doppler shift is positive. When the aircraft is abreast of the radar
               (t = 0) the Doppler shift is zero because the radial component of velocity is
               zero.  Finally,  as  the  aircraft  passes  by  the  radar  (t  >  0)  the  Doppler  shift
               becomes negative, as would be expected for a receding target. This quadratic
               range case is important in synthetic aperture radar and will be revisited in Chap.
               8.
                     The  exponential  term  exp(– j4πR(t)/λ)  in Eq. (2.98)  is  called  the phase
               history of the received signal. This terminology is applied both to the complex

               exponential and to just its phase function (–4πR(t)/λ). The phase history encodes
               the variation of the range between the target and radar during the data collection
               time.  For  the  constant-velocity  example  [Eq.  (2.99)],  the  phase  history  is  a
               linear function of time corresponding to a constant frequency sinusoid, i.e., a
               constant Doppler shift. For the crossing target example of Eq. (2.103), it is a

               quadratic  function  of  time,  producing  a  Doppler  shift  sinusoid  having  a
               frequency  that  varies  linearly  with  time.  Other  radar-target  motions  will
               produce other functional forms for the phase history.
                     More generally, the term phase history can refer to the variation of phase
               (or the corresponding complex exponential) in any dimension of the radar data.
               Two  other  common  uses  are  to  describe  the  fast-time  phase  function  of  a
               frequency- or phase-modulated waveform or the spatial phase variation across

               the face of an array antenna at a fixed time. As will be seen, the phase history is
               central to radar signal processing. The design of many important radar signal
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