Page 406 - Fundamentals of Radar Signal Processing
P. 406

the  target  signals  become  the  dominant  components.  Subsequent  finite

               wordlength processing will adapt the dynamic range to the targets rather than the
               now-suppressed clutter. In the increasingly common floating point processors,
               dynamic range is less of an issue.


               5.5.2   Transient Effects
               All of the discussion in this chapter has assumed a steady-state scenario in the
               sense that the clutter spectrum is stationary and that filter transient effects have

               been  ignored.  In  range-ambiguous  medium  and  high  PRF  modes  the  received
               signal  sample  in  each  range  bin  contains  contributions  from  multiple  ranges
               because of the multiple contributing pulses. Whenever the radar PRF changes
               several pulses, known as clutter fill pulses, they must be transmitted before a
               steady-state situation is achieved. Here “steady state” means that the physical
               clutter intervals contributing to a given range bin are the same for each pulse so
               that the clutter statistics can be expected to be stationary from one pulse to the

               next.  For  example,  suppose  that  in  steady  state  each  range  gate  contains
               significant  contributions  from L = 4 pulses (four range ambiguities). Then the
               clutter signature in each range bin will reach a steady-state condition only for
               the  fourth  and  subsequent  pulses  in  a  CPI.  This  issue  was  first  discussed  in
               Chap. 4.
                     Steady-state operation of the digital filters used for MTI processing occurs

               when the output value depends only on actual data input values rather than any
               initial (typically zero-valued) samples used to initialize the processing. For FIR
               filters of length N, the first and last N – 1 samples of the complete convolution
               are transient in the sense that the filter impulse response does not fully overlap
               the finite data sequence. These transient output samples are often discarded.
                     These two effects are independent. To see how many pulses are needed in
               total to obtain an M-point non-transient, steady-state sequence y [m], consider
                                                                                            ss
               Fig. 5.34.  Assume P  total  pulses  are  transmitted.  This  sketch  assumes L  =  4
               range ambiguities and a three pulse canceller (N = 3) MTI filter, but is labeled
               for general L and N. The notional data sequence y[m] is shown as ramping up in
               amplitude over the first L samples. While actual data would vary unpredictably
               depending on the clutter scenario, this represents the increasing number of range
               ambiguities present in each sample, stabilizing at four when m = 3 (the fourth

               sample). Recall that the convolution of h and y is given by y [n] = Σ y[m]h[n –
                                                                                       ss
               m]. The three-sample sequence in the figure represents the three-pulse canceller
               filter  coefficients h[n  – m]. (The actual coefficient values would be {+1, –2,
               +1}). It can be seen from the figure that in general the first value of n for which
               the filter coefficients will overlap only with steady-state measured data occurs
               when L – 1 = n – N + 1, i.e. n = L + N – 2 (n = 5 in this example). The last value
               for which this is true occurs when n = P – 1. The number of output samples in

               this interval is M = (P – 1) – (L + N – 2) + 1. Therefore, P = M + L + N – 2
               pulses are needed to obtain M valid outputs for further processing.
   401   402   403   404   405   406   407   408   409   410   411