Page 231 - Schaum's Outline of Theory and Problems of Signals and Systems
P. 231

220              FOURIER ANALYSIS OF TIME SIGNALS AND SYSTEMS                   [CHAP.  5



           E.  Time Reversal:





             Thus,  time  reversal  of  x(t)  produces  a  like  reversal  of  the  frequency  axis  for  X(o).
             Equation (5.53) is readily obtained by setting a = - 1  in  Eq. (5.52).


           F.  Duality (or Symmetry):




             The duality property  of  the  Fourier  transform  has significant  implications. This property
             allows  us  to  obtain  both  of  these  dual  Fourier  transform  pairs  from  one  evaluation  of
             Eq. (5.31) (Probs. 5.20 and 5.22).

           G.  Differentiation in the Time Domain:







             Equation  (5.55)  shows  that  the  effect  of  differentiation  in  the  time  domain  is  the
             multiplication  of  X(w) by jw  in  the frequency domain (Prob. 5.28).


           H.  Differentiation in the Frequency Domain:


                                                            dX(4
                                              (-P)x(t) - ,o

             Equation (5.56) is the dual property of  Eq. (5.55).


           I.  Integration in  the Time Domain:







             Since  integration  is  the  inverse  of  differentiation,  Eq. (5.57) shows  that  the  frequency-
             domain operation corresponding  to time-domain  integration is multiplication  by  l/jw,  but
             an  additional  term  is  needed  to  account  for  a  possible  dc component  in  the  integrator
             output. Hence, unless  X(0) = 0, a dc component is produced by the integrator (Prob. 5.33).


           J.  Convolution:
   226   227   228   229   230   231   232   233   234   235   236