Page 160 - Fundamentals of Radar Signal Processing
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determine the range and angle sampling requirements.



               2.7.2   Variation with Angle
               Now consider the variation in reflectivity with angle for a fixed range, say R .
                                                                                                            0
               Define the range-averaged effective reflectivity












                                                                                                     (2.118)

               This is the reflectivity variation in angle, taking into account the range averaging
               at each angle due to the finite pulse length. Note that in the limit of very fine
               range  resolution,  i.e.,  if  the  pulse  modulation x(2R/c)  → δ (R  – R ),  then
                                                                                                    0
                                                                                          D
                                       ,  that  is,  the  “range-averaged”  reflectivity  would  exactly
               equal the effective reflectivity evaluated at the range of interest R .
                                                                                            0
                     Applying Eq. (2.118) to Eq. (2.117) gives










                                                                                                     (2.119)


               where again symmetry of the antenna pattern has been assumed in the second

               line. Equation (2.119) is a special case of Eq. (2.117) showing that the complex
               voltage  at  the  output  of  a  coherent  receiver  for  a  fixed  range  and  a  scanning
               antenna is approximately the convolution in the angle dimensions of the range-
               averaged effective reflectivity function evaluated at the range R ,                       with
                                                                                           0
                                                            2
               the antenna two-way voltage pattern E (θ, ϕ).
                     As  mentioned  earlier,  the  interpretation  of Eq.  (2.119)  as  a  linear
               convolution is an approximation. Suppose that the elevation angle ϕ is fixed, and
               consider only the variation in azimuth angle θ. Because the integration is over a
               full 2π radians and the integrand is periodic in θ with period 2π, the integration
               over azimuth is a circular convolution of periodic functions.
                     This  would  not  appear  to  be  the  case  if  instead θ  is  fixed  and ϕ varies
               because the integrand is over a range of only π radians. However, one could

               equally well replace Eq. (2.119) as
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