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




          Self Assessment                                                                       Notes

          15.  Solve

                1  2 z  1  z  1  2  z  1  z
                                         0
               x 2  x 2  x 3  x  y 2  y 2  y 3  y
          16.  Solve

                  2 z    2 z
               x 2    y 2    xy
                  x  2   y  2

          20.8 Monge’s Method


          We shall usually take  z as dependent and  x, y as independent variables and throughout this
          chapter we shall denote

            z      z       2 z      2 z         2 z
              by  ,p   by  ,q  2  by  ,r   by s, and    by t.
            x      y       x       x y          y 2

          Monge’s Method of Solving  the Equation

                              Rr Ss Tt = V                                         ...(1)

          where r, s, t have their usual meanings and R, S, T and V are functions of x, y, z, p and q.
          We  know

                                            p     p
                                     dp =    dx    dy
                                            x     y
                                        = r dx s dy

                                            q     q
          and                        dq =    dx    dy
                                            x     y

                                        = s dx + t dy.
          Putting the values of r and t in (1),

                          dp s dy         dq s dx
                       R            . S s T .      = V
                            dx              dy

          or   R dp dy T dq dx Ss dxdy Rs dy  2  Ts dx  2  = V dx dy

          or               (R dp dy T dq dx V dx dy  ) = s (R dy 2  S dx dy T dx 2 )  ...(2)

          If some relation between x, y, z, p, q makes each of the bracketed expressions vanish, the relation
          will satisfy (2); therefore

                                R dy  2  S dx dy T dx 2  = 0                       ...(3)

                             Rdp dy T dq dx V dx dy = 0                            ...(4)



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