Page 37 - Fundamentals of Radar Signal Processing
P. 37

processing  and  because  this  approach  can  unify  concepts  and  results  often

               treated separately.




               1.2   Basic Radar Functions

               Most uses of radar can be classified as detection, tracking,  or imaging. This
               text  addresses  all  three,  as  well  as  the  techniques  of  signal  acquisition  and
               interference reduction necessary to perform these tasks.
                     The  most  fundamental  problem  in  radar  is  detection  of  an  object  or
               physical phenomenon. This requires determining whether the receiver output at

               a  given  time  represents  the  echo  from  a  reflecting  object  or  only  noise.
               Detection  decisions  are  usually  made  by  comparing  the  amplitude A(t) of the
               receiver output (where t represents time) to a threshold T(t), which may be set a
               priori in the radar design or may be computed adaptively from the radar data; in
               Chap. 6 it will be seen why this detection technique is appropriate. The time
               required for a pulse to propagate a distance R and return, thus traveling a total

               distance 2R, is just 2R/c; thus, if A(t) > T(t) at some time delay t  after a pulse is
                                                                                           0
               transmitted, it is assumed that a target is present at range





                                                                                                        (1.1)

               where c is the speed of light.    1

                     Once an object has been detected, it may be desirable to track its location
               or  velocity.  A  monostatic  radar  naturally  measures  position  in  a  spherical
               coordinate system with its origin at the radar antenna’s phase center, as shown
               i n Fig. 1.1.  In  this  coordinate  system,  the  antenna  look  direction,  sometimes
               called  the boresight  direction,  is  along  the +x  axis.  The  angle θ  is  called
               azimuth angle, while ϕ is called elevation angle. Range R to the object follows
               directly from the elapsed time from transmission to detection as just described.
               Elevation  and  azimuth  angle ϕ  and θ  are  determined  from  the  antenna

               orientation, since the target must normally be in the antenna main beam to be
               detected.  Velocity  is  estimated  by  measuring  the  Doppler  shift  of  the  target
               echoes. Doppler shift provides only the radial velocity component, but a series
               of  measurements  of  position  and  radial  velocity  can  be  used  to  infer  target
               dynamics in all three dimensions.
   32   33   34   35   36   37   38   39   40   41   42