Page 381 - A Course in Linear Algebra with Applications
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9.4:  Jordan  Normal  Form               365

             The  functions  Ui can  be  found  by  solving  a  series  of  first
        order  linear  equations,  starting  from  the  bottom  of  the  list.
        Thus  u' n  =  du n  yields  u n  =  c n-\e dx  where  c n _i  is  a  constant.
        The  second  last  equation  becomes

                                                   dx
                                 -  dun-i  =   c n-ie ,
                           u' n_ x
                                                             dx
        which  is  first  order  linear  with  integrating  factor  e~ .  Multi-
                                                         dx
        plying the equation  by this  factor,  we get  (u n-ie~ )'  =  c n _i.
        Hence
                          u n-i  =  (c n _ 2  +  c n-ix)e dx

        where  c n_2  is another  constant.  The  next  equation  yields

                                                         dx
                           -         =  (c n-2  +  c n-ix)e ,
                     u' n_ 2  du n- 2
                                                                  dx
        which  is also  first  order  linear  with  integrating  factor  e~ .  It
        can  be  solved  to  give


                             /      .  c  n - 2  ,  c  n - l  2\  dx
                    U n-2  =  (c n -3  +  ~jr X  +  ~^T X  ) e  '

        where  c n„2  is  constant.  Continuing  in  this  manner,  we  find
        that  the  function  « n _i  is  given  by


                 ^•n—i  —  (Cn — i — 1  i  r~|  X  "T  '  " '  ~r  r.  X  )C  ,
                                      1!             i\
        where the  Cj are constants.  The  original  functions  j/j can  then
        be  calculated  by  using  the  equation  Y  —  SU.

        Example     9.4.10
        Solve  the  linear  system  of  differential  equations  below  using
        Jordan  normal   form:

                              y[   =  3yi  +  y 2
                                   =  -yi  + V2
                              y 2
                                   =
                              y' 3               2y 3
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