Mathematical Methods for Physics and Engineering : A Comprehensive Guide

(Darren Dugan) #1

18.1 LEGENDRE FUNCTIONS


Q 0


Q 1


Q 2


x
− 1

− 1


− 0. 5


− 0. 5


0. 5


0. 5


1


1


Figure 18.2 The first three Legendre functions of the second kind.

the coefficientc 2 of the functionQ(x) in (18.7) to be zero, sinceQ(x) is singular


atx=±1, with the result that the general solution is simply some multiple of the


relevant Legendre polynomialP(x). In this section we will study the properties


of the Legendre polynomialsP(x) in some detail.


Rodrigues’ formula

As an aid to establishing further properties of the Legendre polynomials we now


develop Rodrigues’ representation of these functions. Rodrigues’ formula for the


P(x)is


P(x)=

1
2 !

d
dx

(x^2 −1). (18.9)

To prove that this is a representation we letu=(x^2 −1),sothatu′=2x(x^2 −1)−^1


and


(x^2 −1)u′− 2 xu=0.

If we differentiate this expression+ 1 times using Leibnitz’ theorem, we obtain


[
(x^2 −1)u(+2)+2x(+1)u(+1)+(+1)u()

]
− 2 

[
xu(+1)+(+1)u()

]
=0,
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