Page 295 - Fundamentals of Radar Signal Processing
P. 295

(4.125)

               Figure 4.40 illustrates the linearly stepped frequency waveform.












               FIGURE 4.40   Linearly frequency-stepped waveform.



                     Because  only  simple  pulses  are  used  for  each  constituent  pulse,  the
               instantaneous bandwidth capability of the transmitter and receiver need be only
               on the order of 1/τ Hz. The total bandwidth of the waveform as a whole is M ·
               ΔF. When used with a phase-steered array antenna, the time between pulses can

               be used to reset the phase shifters to update the {a } sequence and maintain a
                                                                             n
               nearly constant steering direction θ  as the effective wavelength changes from
                                                          0
               pulse to pulse. The major disadvantages of this waveform are that it requires a
               pulse-to-pulse tunable transmitter and receiver, and that M PRIs are required to
               collect data over the desired bandwidth instead of just one.
                     The pulse-by-pulse processing viewpoint applied to the constant-frequency
               pulse  burst  waveform  can  be  applied  again  to  analyze  the  matched  filter

               response for the stepped frequency waveform. Suppose the radar is stationary,
               and  a  stationary  target  is  located  at  a  range  corresponding  to  a  delay t   + δt,
                                                                                                       l
               where δt  represents  an  incremental  delay  relative  to  the  nominal  delay t              l
               corresponding to range bin l. Individual pulses are processed through the simple
               pulse matched filter as before, producing the output waveforms (assuming T  =
                                                                                                          M
               0)





                                                                                                     (4.126)

               This output is then sampled at t  = t   + mT  (that  is, t  seconds after the current
                                                                               l
                                                          l
               pulse was transmitted), corresponding to range R = ct /2. The resulting sample
                                                                          l
                                                                                l
               becomes the lth coarse range bin sample for the current pulse






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