Page 213 - Fundamentals of Radar Signal Processing
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(3.44)

               Applying a trigonometric identity for sin(θ – ϕ) and equating terms in sinθ and
               cosθ on both sides of Eq. (3.44) leads to the following solution for a  and a :
                                                                                                21
                                                                                                         22




                                                                                                       (3.45)


               Using Eq. (3.45) in Eq. (3.43) gives the final transformation required







                                                                                                       (3.46)

                     Once the I/Q errors ε, ϕ, γ, and κ are determined, Eq. (3.46) can be used to
               compute a new value Q′ for the quadrature channel sample for each measured I-
               Q sample pair. The difficulty, of course, is in actually determining the errors;
               the  correction  is  then  easy.  The  errors  are  generally  estimated  by  injecting  a
               known pilot signal, usually a pure sinusoid, into the receiver and observing the

               outputs. Details for one specific technique to estimate gain and phase errors are
               given  in  Churchill  et  al.  (1981);  that  paper  also  derives  limits  to  mismatch
               correction (and thus to image suppression) caused by noise, which introduces
               errors into the estimates of ε and ϕ.
                     A  second  method  for  eliminating  I/Q  error  is  based  on  the  idea  of
               transmitting multiple pulses, stepping the starting phase of each pulse through a
               series of evenly spaced values, and then integrating the measured returns. To see

               how this technique works, suppose the input signal in Fig. 3.18 is changed to A
               sin [Ωt + θ (t) + k(2π/N)] for some fixed integer N and variable integer k; i.e.,
               the pulse is one of a series of N pulses, where the initial phase is increased by
               2π/N radians on each successive pulse. The extra phase shift propagates to the
               output signals











                                                                                                       (3.47)

               for k = 0, 1, …, N – 1. The development leading to Eq. (3.36) can be repeated
               to  obtain  the  complex  signal  for  this  case,  which  is  (still  suppressing  the t
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