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                     46  ESSENTIALS OF APPLIED MATHEMATICS FOR SCIENTISTS AND ENGINEERS
                       4.1.2  Ordinary Points and Series Solutions
                       If the point x 0 is an ordinary point the dependent variable has a solution in the neighborhood
                       of x 0 of the form
                                                              ∞
                                                                         n
                                                      u(x) =    c n (x − x 0 )                       (4.3)
                                                             n=0
                       We now illustrate the solution method with two examples.
                       Example 4.1. Find a series solution in the form of Eq. (4.3) about the point x = 0ofthe
                       differential equation

                                                                2
                                                          u + x u = 0                                (4.4)

                       The point x = 0 is an ordinary point so at least near x = 0 there is a solution in the form of
                       the above series. Differentiating (4.3) twice and inserting it into (4.4)
                                                           ∞

                                                                  n−1
                                                     u =      nc n x
                                                          n=0
                                                           ∞

                                                                        n−2
                                                     u =      n(n − 1)c n x
                                                          n=0
                                                ∞                   ∞
                                                              n−2       n+2
                                                   n(n − 1)c n x  +    x   c n = 0                   (4.5)
                                                n=0                n=0
                       Note that the first term in the u series is zero while the first two terms in the u series are zero.


                       We can shift the indices in both summations so that the power of x is the same in both series
                       by setting n − 2 = m in the first series.
                           ∞                   ∞                           ∞
                                        n−2                           m                          m
                             n(n − 1)c n x  =      (m + 2)(m + 1)c m+2 x =    (m + 2)(m + 1)c m+2 x  (4.6)
                          n=0                 m=−2                        m=0
                       Noting that m is a “dummy variable” and that the first two terms in the series are zero the series
                       can be written as

                                                      ∞
                                                                          n
                                                        (n + 2)(n + 1)c n+2 x                        (4.7)
                                                     n=0
                            In a similar way we can write the second term as

                                                      ∞           ∞
                                                            n+2           n
                                                         c n x  =    c n−2 x                         (4.8)
                                                     n=0          n=2
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