Page 355 - Schaum's Outline of Theory and Problems of Signals and Systems
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342        FOURIER ANALYSIS OF DISCRETE-TIME SIGNALS AND SYSTEMS  [CHAP.  6



            6.46.  Consider designing a discrete-time LTI system with system function  HJz) obtained by
                  applying  the  bilinear  transformation  to a  continuous-time  LTI  system  with  rational
                  system function  H,(s). That is,




                  Show that a stable, causal continuous-time system will  always lead  to a stable, causal
                  discrete-time  system.
                     Consider the bilinear  transformation of  Eq. (6.183)






                  Solving Eq. (6.188) for z, we  obtain





                  Setting s = jw  in  Eq. (6.1891, we  get





                  Thus, we see that the jw-axis of the s-plane is transformed  into the unit circle of  the  z-plane.
                  Let

                                             z =re'"    and    s =a + jo
                  Then from Eq. (6.188)





                                                  r2- 1             2r sin $2
                                              1 +r2+2rcosR +'1+r2+2rcos~

                  Hence,





                                                    2      2r sin R
                                                w=-
                                                    T,  1 +r2+2rcosR

                  From Eq. (6.191a) we see that if  r < 1, then  a < 0, and if  r > 1, then  cr > 0. Consequently, the
                  left-hand  plane  (LHP)  in  s  maps  into the  inside  of  the  unit  circle  in  the  z-plane,  and  the
                  right-hand  plane  (RHP) in  s  maps  into  the  outside  of  the  unit  circle  (Fig.  6-32). Thus,  we
                  conclude that a stable, causal continuous-time system will lead to a stable, causal discrete-time
                  system  with  a bilinear  transformation (see Sec. 3.6B and  Sec. 4.6B). When  r = 1,  then  o = 0
                  and
                                                   2   sin 0     2    R
                                              w=-             = -tan-
                                                   T, I  + cos R   T,   2
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