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Unit 20: Higher Order Equations with Constant Coefficients and Monge’s Method




          In case of repeated factors                                                           Notes
                                                2
                                     (D mD     ) z = 0                             ...(1)
          or               (D mD      )(D mD    )z = 0

          let                      (D mD     )z  ,

                                 Then, (D mD    )                             [from (1)]

          or                                       = e ax  (y mx )

          or                          (D mD     )z = e ax  (y mx );
                                                         1

                                                                   y
                                                            )}
                           z = e (mD  )x  {e  (mD  )x  e ax  1  (y mx dx  ( )
                                                ax
                                          y
                                                         y
                             = e (  mD  ) x  ( )dx  e e (mxD  )  2 ( )
                             = e  x .x  1 (y mx ) e  x  2 (y mx )
                                                 r
          Similarly proceeding in the case of  (D mD  ) z  0,  we have
                                             x
                                                                          x r
                                                          x
                           z = e  x  (y mx ) e x  (y mx ) e x 2  (y mx ) ... e x  1  (y mx )
                                   1                          3                r
          The Particular Integral
          The  methods  for  obtaining particular  integrals  of  non-homogeneous  partial  differential
          equations are very similar to those used in solving linear equation with constant coefficients.
          Note: It can be easily shown that

                  1    ax by  e ax by
          I.          e
               F ( ,D  )    F ( , )
                 D
                               b
                              a
               provided  ( , ) 0.F a b
                  1
          II.         sin(ax by ) or cos(ax by )
               F ( ,D  )
                 D
               is obtained by putting  D 2  a  2 , DD  ab  and  D  2  b 2 ,  provided the denominator is
               not zero.

                  1    m n          1  m n
                            F
                              D
          III.        x y   [ ( ,D  )] x y
               F ( ,D  )
                 D
               which can be evaluated after expanding  [ ( ,F D D  )]  1   in ascending powers of D or D .
                  1    ax by
                           V
          IV.         (e   . )
                 D
               F ( ,D  )
                          1
                ax by
               e                  .V
                    F {(D a ).(D  b )}


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