Page 93 - Fundamentals of Radar Signal Processing
P. 93

(2.11)


               Equation  (2.11)  is  one  simple  form  of  the radar  range  equation.  It  relates

               received echo power to fundamental radar system and target parameters such as
               transmitted power, operating frequency, and antenna gain; radar cross section;
               and range. Because the power of the radar signal is proportional to the square of
               the electric field amplitude, the range equation also serves as a model of the
               amplitude  of  the  target  and  clutter  components  of  the  signal.  Note  that  all

               variables in Eq. (2.11) are in linear units, not decibels, even though several of
               the  parameters  are  often  specified  in  decibels;  frequent  examples  include  the
               atmospheric losses, antenna gain, and RCS. Also note that P  is instantaneous,
                                                                                         r
               not average, received power. Finally, realize that for a scatterer at range R, the
               backscattered EM wave will be received with a time delay of 2R/c seconds
               after transmission.
                     As  an  example,  consider  an  X-band  (10-GHz)  radar  with  a  peak
               transmitted power of 1 kW and a pencil beam antenna with a 1° beamwidth, and

                                                                                                          2
               suppose an echo is received from a jumbo jet aircraft with an RCS of 100 m  at
               a range of 10 km. The received power can be determined using Eq. (2.11). The
               antenna gain can be estimated from Eq. (1.10) to be G = 26,000/(1)(1) = 26,000
                                                                                               –2
                                                                      8
                                                                                  9
               = 44 dB. The wavelength is λ = c/F = 3 × 10 /10 × 10  = 3 × 10  m = 3 cm.
               Assuming atmospheric and system losses are negligible, the received power is





                                                                                                       (2.12)

               Even though this example is a large target at short range, the received power is
               only 3.07 nW, nearly 12 orders of magnitude less than the transmitted power!
               Nonetheless, this signal level is adequate for reliable detection in many cases.
               This  example  illustrates  the  huge  dynamic  ranges  observed  in  radar  between

               transmitted and received signal powers.
                     An  important  consequence  of Eq.  (2.11)  is  that  for  a  point  target,  the
               received power decreases as the fourth power of range from the radar to the
               target.  Thus,  the  ability  to  detect  a  target  of  a  given  radar  cross  section
               decreases rapidly with range. Range can be increased by increasing transmitted
                                                 4
               power, but because of the R  dependence, the power must be raised by a factor
               of 16 (12 dB) just to double the detection range. Alternatively, the antenna gain
               can be increased by a factor of 4 (6 dB), implying an increase in antenna area by
               a factor of 4. On the other hand, designers of “stealth” aircraft and other target
               vehicles must reduce the RCS σ by a factor of 16 in order to halve the range at
               which they can be detected by a given radar system.
                     The range equation is a fundamental radar system design and analysis tool.
               More  elaborate  or  specialized  versions  of  the  equation  can  be  formulated  to
   88   89   90   91   92   93   94   95   96   97   98