Page 282 - Schaum's Outline of Theory and Problems of Advanced Calculus
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CHAP. 11]                         INFINITE SERIES                               273

                                                          1          1                            1
                                                          X         X                            X
                                                               n
                                                                          n
                     Theorem 14.  Two power series, for example,  a n x and  b n x , can be multiplied to obtain  c n x n
                                                          n¼0       n¼0                          n¼0
                     where
                                              c n ¼ a 0 b n þ a 1 b n 1 þ a 2 b n 2 þ     þ a n b 0  ð11Þ
                     the result being valid for each x within the common interval of convergence.
                                                1
                                               X     n                            n
                     Theorem 15.  If the power series  a n x is divided by the power series  b n x where b 0 6¼ 0, the quotient
                                                n¼0
                     can be written as a power series which converges for sufficiently small values of x.
                                       1                           1
                                      X                            X
                                            n
                                                                        n
                     Theorem 16.  If y ¼  a n x , then by substituting x ¼  b n y ,we can obtain the coefficients b n in
                                       n¼0                         n¼0
                     terms of a n . This process is often called reversion of series.

                     EXPANSION OF FUNCTIONS IN POWER SERIES
                        This section gets at the heart of the use of infinite series in analysis.  Functions are represented
                     through them. Certain forms bear the names of mathematicians of the eighteenth and early nineteenth
                     century who did so much to develop these ideas.
                        A simple way (and one often used to gain information in mathematics) to explore series representa-
                     tion of functions is to assume such a representation exists and then discover the details.  Of course,
                     whatever is found must be confirmed in a rigorous manner.  Therefore, assume
                                                                  2              n
                                       f ðxÞ¼ A 0 þ A 1 ðx   cÞþ A 2 ðx   cÞ þ     þ A n ðx   cÞ þ
                        Notice that the coefficients A n can be identified with derivatives of f .In particular
                                                             1              1
                                                     0          00            f  ðnÞ ðcÞ; ...
                                                             2!             n!
                                       A 0 ¼ f ðcÞ; A 1 ¼ f ðcÞ; A 2 ¼  f ðcÞ; ... ; A n ¼
                        This suggests that a series representation of f is
                                                        1                 1
                                             0             00      2        f  ðnÞ    n
                                                       2!                 n!
                                 f ðxÞ¼ f ðcÞþ f ðcÞðx   cÞþ  f ðcÞðx   cÞ þ     þ  ðcÞðx   cÞ þ
                        A first step in formalizing series representation of a function, f , for which the first n derivatives exist,
                     is accomplished by introducing Taylor polynomials of the function.
                                                        P 1 ðxÞ¼ f ðcÞþ f ðcÞðx   cÞ;
                                                                     0
                                          P 0 ðxÞ¼ f ðcÞ
                                                                  1
                                                                             2
                                                                    00
                                                       0           f ðcÞðx   cÞ ;
                                                                 2!
                                          P 2 ðxÞ¼ f ðcÞþ f ðcÞðx   cÞþ
                                                                      1
                                                                        f
                                                       0                 ðnÞ      n
                                                                      n!
                                          P n ðxÞ¼ f ðcÞþ f ðcÞðx   cÞþ     þ  ðcÞðx   cÞ           ð12Þ
                     TAYLOR’S THEOREM
                        Let f and its derivatives f ; f ; ... ; f  ðnÞ  exist and be continuous in a closed interval a   x   b and
                                                00
                                              0
                     suppose that f  ðnþ1Þ  exists in the open interval a < x < b. Then for c in ½a; bŠ,
                                                      f ðxÞ¼ P n ðxÞþ R n ðxÞ;
                     where the remainder R n ðxÞ may be represented in any of the three following ways.
                        For each n there exists   such that
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