Page 312 - A Course in Linear Algebra with Applications
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296           Chapter  Eight:  Eigenvectors  and  Eigenvalues

                 Finally,  suppose  that  initial  conditions  j/i (0)  =  1  and
            V2 (0)  =  0  are  given.  We  can  find  the  correct  values  of  c\  and
               by substituting  t  =  0 in the expressions  for  y\  and  j/2, to  get
            c 2
                                                                           2x
            ci  =  1 and  C2 =  — 1.  The  required  solution  is  y\  =  (1 — x)e
                             2x
            and  ?/2 =  — x  e .
                 The  next  application  is one  of  a  military  nature.
            Example    8.3.4
            Two  armored   divisions  A  and  B  engage  in  combat.  At  time  t
            their  respective  numbers  of tanks  are  a(t)  and  b(t).  The  rate
            at  which  tanks  in  a  division  are  destroyed  is  proportional  to
            the  number  of  intact  enemy  tanks  at  that  instant.  Initially
            A  and  B  have  ao  and  bo tanks  where  ao  >  &o-  Predict  the
            outcome  of the  battle.
                 According  to  the  information  given,  the  functions  a  and
            b satisfy  the  linear  system
                                       a'   =  -kb
                                       b'  =   -ka

            where  k  is some  positive constant.  Here the  coefficient  matrix
            is
                                            0    -k'
                                  A
                                   ~    '  -k    0
            The  characteristic  equation  is  x 2  —  k 2  =  0,  so the  eigenvalues
            are  k  and  —k and  A  is diagonalizable.  It  turns  out  that






            where  S  =  (          .  If  we  set  F  =    ,  the  system  of

            differential  equations  becomes  Y'  =  AY.  On   writing  U  =
              X
            S- Y,   we get  U'  =  DU.  This  is the  system
                                       u'   =   ku
                                       v'   =  —kv
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