Page 76 - Schaum's Outline of Theory and Problems of Signals and Systems
P. 76

CHAP.  21                 LINEAR TIME-INVARIANT SYSTEMS                               65



              where A  is the eigenvalue of  T associated with  zn. Setting x[n] = zn in  Eq. (2.391, we  have



                                               k= -m
                                     = H(z)zn = Azn                                           (2.51)
                                                          rn
              where                         A  = H(z) =  x h[k] zPk                           (2.52)
                                                        k= -ra
              Thus, the eigenvalue of  a discrete-time LTI system associated with the eigenfunction zn is
              given by  H(z) which is a complex constant whose value is determined by  the value of z via
              Eq. (2.52). Note from Eq. (2.51) that  y[O] = H(z) (see Prob. 1.45).
                 The above results underlie the definitions of  the z-transform and discrete-time Fourier
              transform which will be discussed in  Chaps. 4 and 6.



            2.9  SYSTEMS DESCRIBED BY  DIFFERENCE EQUATIONS
                 The  role  of  differential equations in  describing continuous-time  systems is  played  by
              difference equations  for discre te-time systems.

            A.  Linear Constant-Coefficient Difference Equations:

                 The discrete-time  counterpart  of  the  general differential equation (2.25) is  the  Nth-
              order linear constant-coefficient difference equation given by
                                          N                M



              where coefficients a,  and b,  are real constants. The order N refers to the largest delay of
              y[n]  in  Eq.  (2.53).  An  example  of  the  class  of  linear  constant-coefficient  difference
              equations  is  given  in  Chap.  I  (Prob.  1.37). Analogous  to  the  continuous-time  case,  the
              solution  of  Eq.  (2.53)  and  all  properties  of  systems,  such  as  linearity,  causality,  and
              time-invariance,  can  be  developed  following  an  approach  that  directly  parallels  the
              discussion for differential equations. Again we  emphasize that the system described by  Eq.
              (2.53) will be causal and LTI if  the system is initially at rest.


            B.  Recursive Formulation:
                 An  alternate and  simpler approach  is  available  for the  solution of  Eq.  (2.53). Rear-
              ranging Eq. (2.53) in the form





              we obtain a formula to compute the output at time n in terms of  the present input and the
              previous values of  the input and output. From Eq. (2.54) we see that the need for auxiliary
              conditions is  obvious and  that  to calculate  y[n] starting  at  n = no, we  must  be  given  the
             values of  y[n,, - 11,  y[no - 21,. . . , y[no - N] as well as the input  x[n] for n 2 n,, - M. The
              general  form  of  Eq.  (2.54) is  called  a  recursiue  equation  since  it  specifies  a  recursive
              procedure  for determining the output in  terms of  the  input  and  previous outputs.  In  the
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