Page 207 - Fundamentals of Radar Signal Processing
P. 207

The 3-dB beam-width of an aperture antenna is of the form (Balanis, 2005)






                                                                                                       (3.31)

               For the uniformly illuminated case, k = 0.89. Combining Eqs. (3.30) and (3.31)
               gives






                                                                                                       (3.32)

               For k  =  0.89,  this  gives  a  Nyquist  sampling  rate  of  0.56  times  the  3-dB
               beamwidth,  or  1.8  samples  per  3-dB  beamwidth.  In  practice,  many  systems
               sample in angle at approximately one sample per 3-dB beamwidth. The search
               space is then undersampled in angle, at least according to the Nyquist criterion.

                     While derived for the uniformly illuminated aperture, these results apply to
               all aperture antennas. For a finite aperture of size D, different antenna patterns
               (for  instance,  with  lower  sidelobes  at  the  expense  of  a  wider  mainlobe)  are
               obtained by changing the aperture illumination function, typically by tapering it
               in a manner similar to windowing operations in signal processing. The Fourier

               transform of these antenna power patterns will still be the autocorrelation of the
               corresponding  illumination  function.  Since  the  illumination  function  still  has
               finite support, its autocorrelation will still be limited to a width of 2α in s, as
               shown  in Fig. 3.17; only the detailed shape of the function will change. Thus,
               Eq. (3.32)  applies  for  any  finite  aperture  antenna.  The  difference  is  that  the
               factor k will be different for different illumination functions. Lower sidelobe
               antennas will have values of k in the range of approximately 1.4 to 2.0, giving
               corresponding Nyquist sampling rates on the order of 2.8 to four samples per 3-

               dB beamwidth for low sidelobe antennas.
                     For  a  rotating  radar,  the  angular  sampling  rate  of Eq.  (3.31)  implies  a
               lower bound on PRF. Suppose the rate of rotation is Ω  radians per second. In
                                                                                 0
               order that successive pulses be transmitted in directions differing by no more
               than the T  of (3.31), the PRI and PRF must satisfy
                          θ





                                                                                                       (3.33)


                     Equations (3.33)  and (3.9) illustrate a conflict between volume coverage

               and search rate in a rotating search radar. For a given antenna design, θ  and k
                                                                                                      3
               are fixed. Then, increasing the sweep rate Ω  will increase the volume search
                                                                     0
               rate,  but  will  also  require  an  increased  PRF;  but  a  higher  PRF  reduces  the
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