Page 306 - A Course in Linear Algebra with Applications
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2 9 0          Chapter  Eight:  Eigenvectors  and  Eigenvalues

                 If  a  set  of  n  initial  conditions  is  given,  there  is  in  fact  a
            unique  solution  of the  system  satisfying  these  conditions.  For
            an  account  of  the  theory  of  systems  of  differential  equations
            the  reader  may  consult  a  book  on  differential  equations  such
            as  [15] or  [16].  Here  we are  concerned  with  methods  of  finding
            solutions,  not  with  questions  of  existence  and  uniqueness  of
            solutions.
                 Suppose   that  the  coefficient  matrix  A  is  diagonalizable,
                                                                     1
            so  there  is  an  invertible  matrix  S  such  that  D  =  S~ AS  is
            diagonal,  with  diagonal  entries  d\,...,  d n  say.  Here  of  course
            the  di  are the  eigenvalues  of  A.  Define

                                               X
                                       U  =   S- Y.
            Then   Y  — SU   and  Y'  =  SU'  since  S  has  constant  entries.
            Substituting  for  Y  and  Y'  in the equation  Y'  =  AY,  we obtain
            SU'  =  ASU,  or

                                         1
                                U'  =  {S~ AS)U   =  DU.
            This  is  a system  of  linear  differential  equations  for  u\,...,  u n,
            the  entries  of  U.  It  has  the  very  simple  form

                                               d\Ui
                                       u' 2    d 2u 2




            The  equation  u\  =  diUi  is  easy  to  solve  since  its  differential
            form  is
                                     d(ln  Ui) =  di.

            Thus   its  general  solution  is  u^  =  Cie diX  where  ci  is  a  con-
            stant.  The  general  solution  of the  system  of  linear  differential
            equations  for  u\,...,  u n  is  therefore


                            ui  =cie  d i a ;  ,  ...  ,u n  =  c ne dnX .
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