Page 189 - Fundamentals of Radar Signal Processing
P. 189

spectrum via a DTFT of the slow time signal in the appropriate range bin, the

               blind  Doppler  and  velocity  intervals  are F   =  3  kHz  and v   =  45  m/s,
                                                                      Db
                                                                                              b
               respectively. The unambiguous Doppler shift and velocity are then 1.5 kHz and
               22.5 m/s. The DTFT will be interpreted as covering [–1.5, +1.5) kHz and [–
               22.5, +22.5) m/s. The target’s Doppler shift and velocity are outside of these
               intervals and will therefore be aliased into them. With n = 2 in Eq. (3.8), it is
               seen that the apparent Doppler and velocity are F  = 0.67 kHz and v  = +10
                                                                            Da
                                                                                                    a
               m/s.
                     The PRF also sets a limit on the range swath. In particular, the maximum
               range from which the end of the echo of one pulse can be received before the
               next pulse is transmitted is the unambiguous range R . It must satisfy 2R /c + τ
                                                                              ua
                                                                                                      ua
               < T, so










                                                                                                        (3.9)

               The approximation in the second line applies when T   τ and is often cited as
               the definition of R . The far edge of the sampled range swath (R   in Fig. 3.1)
                                     ua
                                                                                              2
               must be limited to R  m or less so the full pulse echo from a scatterer at R  is
                                                                                                          2
                                       ua
               received before the next pulse is transmitted.
                     In  general,  it  is  desirable  to  be  able  to  choose  the  PRF  to  provide  the
               desired unambiguous range and Doppler bandwidth simultaneously. However,
               unambiguous  range  increases  with  decreasing  PRF,  while  the  blind  Doppler
               interval  increases  with  increasing  PRF. Equations  (3.7)  and (3.9)  can  be
               combined to make this explicit:






                                                                                                       (3.10)

               Because the right-hand side of either version of Eq. (3.10) is a constant for a
               given  RF,  increasing R   requires  decreasing F   or v . As  a  result,  in  many
                                                                         Db
                                                                                  b
                                           ua
               situations it is not possible to simultaneously obtain the desired unambiguous
               velocity interval and unambiguous range with a single PRF.
                     To  illustrate  the  effect  of  the  PRF  on  range  measurements  more  fully,
               consider the idealized signals of Fig. 3.6a. In the first line, a pulse is transmitted
               at time t = 0. It is assumed that there are two targets present at ranges R  and R ,
                                                                                                    1
                                                                                                            2
               and that the PRF is such that the unambiguous range falls between these two.
               The target echoes occur 2R /c and 2R /c seconds after transmission, as shown.
                                                             2
                                                1
               Now suppose a second pulse is transmitted at a PRI T = 2R /c. Assume τ   T
                                                                                       ua
   184   185   186   187   188   189   190   191   192   193   194