Page 751 - Mechanical Engineers' Handbook (Volume 2)
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742   State-Space Methods for Dynamic Systems Analysis

                          Table 5 Solution of the State-Space Equations for Linear, Discrete-Time Systems
                                           Time-Invariant System           Time-Varying System
                                            [Eqs. (12) and (13)]            [Eqs. (10) and (11)]
                                     x(k)    (k   k )x(k )          x(k)    (k, k )x(k )
                                                0  0                         0  0
                                                (k   m   1)Gu(m)               (k, m   1)G(m)u(m)
                                                                           k 1
                                            k 1
                                            m k 0                          m k 0
                          Solution
                                     y(k)   C (k   k )x(k )         y(k)   C(k) (k, k )x(k )
                           k   k 0               0  0                           0  0
                                               [C (k   m   1)Gu(m)]           [C(k) (k, m   1)G(m)u(m)]
                                            k 1
                                                                           k 1
                                            m k 0                          m k 0
                                            Du(k)                          D(k)u(k)
                          State       (k   k 0 )   F k k 0  k   k 0
                                                                             k 1
                           transition             or                       
   F(l)  k   k 0
                                                       1
                                              1
                           matrix       (k)   L [z(zI   F) ]         (k, k )    l k  k   k 0
                                                                        0
                                                                             I
                          Properties   (0)   I                       (k 0 , k 0 )   I
                           of state   (k 1   k 2 )    (k 1 ) (k 2 )   (k 2 , k 1 ) (k 1 , k 0 )    (k 2 , k 0 )
                                             1
                                                                              1
                           transition   (k)     ( k)                 (k 1 , k 2 )     (k 2 , k 1 )
                           matrix    when the inverse exists        when the inverse exists
                                                       (k   k )   F k k 0                     (50)
                                                             0
                          Numerical computation of  (k   k ) is thus straightforward. Analytical evaluation of  (k
                                                      0
                            k ) using Eq. (50) is feasible if F is in the diagonal or nondiagonal Jordan canonical form.
                             0
                          If F is a diagonal matrix with diagonal elements equal to its eigenvalues z , i   1,..., n,
                                                                                     i
                          then
                                                              z k 1  z k  0
                                                   (k)   F       0 2                          (51a)
                                                         k
                                                                       z k n
                          If F is in the nondiagonal Jordan canonical form, analytical evaluation of  (k) is only slightly
                          more complex. If the transformation matrix T [Eq. (17)] was used to obtain the diagonal or
                                                                                             1
                          nondiagonal Jordan matrix F, the transition matrix, for the original state vector T x,is
                            1
                              k
                          T F T.
                             An alternative analytical evaluation of the transition matrix uses the relationship
                                                                      1
                                                     (k)   L [z(zI   F) ]                    (51b)
                                                            1
                                 1
                          where L  denotes the inverse z-transform. This method is useful only for low-order systems
                          because of the need for inverting the matrix zI   F, which has symbolic elements. The
                          matrix inversion is particularly simple if F is in the diagonal or Jordan canonical form. As
                          for continuous-time systems, the matrix inversion can be avoided altogether by using sim-
                                                                                   2
                          ulation diagrams of the discrete-time system and block diagram reduction to directly deter-
                                                        1
                          mine elements of the matrix (zI   F) .
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