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dy
                                                     Unit 6: Existence Theorem for the Solution of the Equation    = f(x, y)
                                                                                                      dx


                            x  3  5  x 6  x 9                                                   Notes
                      = 1        x
                            2  40    60  192
                         1   x  3 3  x  3    7     3
                    z =       x         x  4  x  5  x 8  dx
                         2   0   2  2  8    40    64
                         1  3  4  x  5  3  8  7  9  x 12
                      =      x         x     x
                         2  8    10  64   360    256
          and so on. So the series solution of y and z are convergent for x < 1.

          Self-Assessment

          1.   Solve the differential equation
                  dy
                      = y
                  dx
               under the initial conditions y = 1 for x = 1 by the method of successive approximations.
          2.   Solve the differential equation
                  dy
                      = x + y  2
                  dx
               under the initial condition y = 0 when x = 0.

          6.3 Remark on Approximate Solutions

          On letting m     in equation (15), we obtain

                               (K  ) k
                       x
                 x
                y ( )  y  ( )  K
                      n                                                            ...(1)
                            k  n
          for |x   x |  . The equation (17) is an estimate of the error of the  nth approximate solution
                  0
          y (x). The method of successive approximation may be used, in principle. However this method
           n
          is not always practical because it requires one to repeat the evaluation of indefinite integrals
          many times.
          We shall now consider another method which is sometimes rather useful. Suppose that g(x, y) is
          a suitable approximation to  f(x, y)  such that we can find the solution  z(x) of the differential
          equation

                   dz
                      = g(x, y)                                                    ...(2)
                  dx
          On the interval |x   x |   satisfying the initial condition z(x ) = y . We put
                            0                               0   0
                                     y
                           f
                            x
                              y
                                   x
                  SUP     | ( , ) g ( , )|                                        ...(3)
                      x
                     ( , ) D
                       y
                        
          Let y(x) be the unique solution of the differential equation
                  dy
                      = f(x, y)                                                    ...(4)
                  dx
          on the interval |x   x |  h satisfying the initial condition y(x ) = y . Then from (2) it follows that
                           0                               0   0
                          x
                                       z
                                           dt
                                         t
                                      t
                            f
             y(x)   z(x) =  ( ( , ( ))  g ( , ( )) .
                              t
                                t
                               y
                          0 x
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