Page 70 - Essentials of applied mathematics for scientists and engineers
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book   Mobk070    March 22, 2007  11:7








                     60  ESSENTIALS OF APPLIED MATHEMATICS FOR SCIENTISTS AND ENGINEERS



























                       FIGURE 4.1: Bessel functions of the first kind


                            Bessel functions of the first and second kinds of order zero are particularly useful in
                       solving practical problems (Fig. 4.1). For these cases

                                                             ∞
                                                                       x
                                                                (−1) k     2k

                                                     J 0 (x) =                                      (4.80)
                                                                 (k!) 2  2
                                                             k=0
                       and
                                                                 ∞      k+1
                                                                    (−1)
                                                                                2k
                                               Y 0 = J 0 (x)ln(x) +        φ(k)x                    (4.81)
                                                                     2k
                                                                    2 (k!) 2
                                                                k=1
                       The case of ν  = n. Recall that in (4.70) if ν is not an integer, a part of the denominator is

                                                  (1 + ν)(2 + ν)(3 + ν) ... (n + ν)                 (4.82)


                       We were then able to use the familiar properties of factorials to simplify the expression for
                       J n (x). If ν  = n we can use the properties of the gamma function to the same end. The gamma
                       function is defined as
                                                               ∞

                                                                    e dt
                                                        (ν) =    t ν−1 −t                           (4.83)
                                                              0
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