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Unit 12: Sturm Comparison and Separation Theorems




          This gives the second solution of (2) as                                              Notes

                                          x  1   1       1
                                  u 2 ( ) x  2               dt
                                    x
                                            t  2(1 t )  2(1 t )
                                                 x
                                     1  1    1 t    x    1 x
                                 x       log          log       1,
                                     t  2   1 t     2    1 x
          and hence the general solution is

                                              x    1 x
                                    y = Ax + B   log     1 .
                                              2    1 x

          Self Assessment

          1.   Use the reduction of order method to find the second independent solution of the equation

                                           2
                                          d y  2 dy  y  0
                                          dx  2  x dx
                                    1
               with the solution u (x) = x  sin x
                              1
          12.3 The Method of Variation of Parameters

          Let’s now  consider how  to find  the particular  integral given  the complementary function,
          comprising u (x) and u (x). As the name of this technique suggests, we take the constants in the
                     1      2
          complementary function to be variable, and assume that
                                       y = c (x)u (x) + c (x)u (x)
                                          1   1     2  2
          Differentiating, we find that

                                   dy   du 1   dc 1  du 2  dc  2
                                      c 1    u 1   c 2   u 2
                                   dx    dx    dx    dx     dx
          We will choose to impose the condition
                                         dc     dc
                                       u 1  1  u 2  2  0,                          ...(4)
                                          dx    dx
          and thus have

                                         dy   du     du
                                            c 1  1  c 2  2  ,
                                         dx    dx    dx
          which, when differentiated again, yields
                                 2
                                        2
                                                      2
                                d y  c  d u 1  du dc  1  c  d u 2  du dc 2
                                              1
                                                             2
                                dx 2  1  dx 2  dx dx  2  dx 2  dx dx
          This form can then be substituted into the original differential equation to give
                                    2
                     2
                    d u   du dc    d u  du dc       du    du
                  c 1  1   1   1  c  2  2  2  2  a c 1  1  c 2  2  a 0  (c u  c u  ) f  .
                                                                       2 2
                                                                  1 1
                                                1
                     dx  2  dx dx  dx  2  dx dx      dx    dx
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