Mathematical Methods for Physics and Engineering : A Comprehensive Guide

(Darren Dugan) #1

SPECIAL FUNCTIONS


J 0


J 1


J 2


246810


x

− 0. 5


0. 5


1


1. 5


Figure 18.5 The first three integer-order Bessel functions of the first kind.

this is given by


J 0 (x)=

∑∞

n=0

(−1)nx^2 n
22 nn!Γ(1 +n)

=1−

x^2
22

+

x^4
2242


x^6
224262

+···.

In general, however, ifνis a positive integer then the solutions of the indicial

equation differ by an integer. For the larger root,σ 1 =ν, we may find a solution


Jν(x), forν=1, 2 , 3 ,..., in the form of the Frobenius series given by (18.79).


Graphs ofJ 0 (x),J 1 (x)andJ 2 (x) are plotted in figure 18.5 for realx.Forthe


smaller root,σ 2 =−ν, however, the recurrence relation (18.78) becomes


n(n−m)an+an− 2 =0 forn≥ 2 ,

wherem=2νis now anevenpositive integer, i.e.m=2, 4 , 6 ,.... Starting with


a 0 = 0 we may then calculatea 2 ,a 4 ,a 6 ,..., but we see that whenn=mthe


coefficientan is formally infinite, and the method fails to produce a second


solution in the form of a Frobenius series.


In fact, by replacingνby−νin the definition ofJν(x) given in (18.79), it can

be shown that, for integerν,


J−ν(x)=(−1)νJν(x),
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