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Unit 19: Jacobi’s Method for Solving Partial Differential Equations




                                                                                                Notes
                                            ,
                                          ,
                                 F x 1 ,x x p p p 3  =  2                         ...(3)
                                       ,
                                               ,
                                      2
                                 2
                                         3
                                           1
                                              2
          Here   and   are arbitrary constants. These equations are such that p , p , p  can be found from
                1    2                                            1  2  3
          (1), (2), (3) as functions of x , x , x  that make the equation
                                1  2  3
                                     dz = p dx 1  p dx 2  p dx 3                   ...(4)
                                                  2
                                            1
                                                        3
          integrable, for which the conditions are
                                     p 2  =  2 z   p 1  ,  p 3  2 z  p 1  ,  p 3  p 2  ...(5)
                                     x 1    x x  2  x 2  x 1  x x  3  x 1  x 2  x 3
                                                            1
                                             1
          Now by differentiating (1) partially with respect to x , keeping x , x  constant, but regarding p ,
                                                    1         2  3                   1
          p , p , as dependent functions of x , x , x , we get
           2  3                      1  2  3
                         F    F  p 1  F  p 2  F  p 3  = 0                          ...(6)
                         x 1  p 1  x 1  p 2  x 1  p 3  x 1
          Similarly
                         F   F  p    F  p    F  p
                          1   1  1    1  2   1  3  = 0                             ...(7)
                         x 1  p 1  x  1  p 2  x 1  p 3  x 1
                                  F                    F
          Multiplying equation (6) by   1   and equation (7) by   ,  and subtracting we get
                                  p 1                  p 1
                       , F F 1  , F F 1  p 2  , F F 1  p 3
                      x  ,p   p  ,p  x   p  ,p  x  = 0                             ...(8)
                       1  1    2  1  1    3  1  1
          where
                     , F F 1   denotes "Jacobian"   F F 1  F F 1  .
                    x 1 ,p 1             x 1  p 1  p 1  x 1

          Similarly, like (8) we get

                       , F F   , F F  p    , F F  p
                        1        1   1      1   3
                     x  ,p    p  ,p  x   p  ,p  x  = 0                             ...(9)
                      2  2     1  2  2    3  2  2
          and

                       , F F 1  , F F 1  p 1  , F F 1  p 2
                      x  3 ,p 3  p 1 ,p 3  x 3  p 2 ,p 3  x 3  = 0                ...(10)

          Add equation (8), (9) and (10) and noting that two pairs of terms are:

                            , F F  p   , F F  p   2 z    , F F   , F F
                             1   2      1    1            1        1   0
                          p  ,p  x   p  ,p  x   x x    p  ,p    p  ,p
                           2  1  1    1  2   2   1  2   2  1     1  2
          Similarly two other pairs of terms also vanish, leaving

                             , F F 1  , F F 1  , F F 1  = 0                       ...(11)
                            x 1  ,p 1  x  2 ,p 2  x 3  ,p 3




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