Legendre differential equation
From Wikiversity
The Legendre differential equation is the second order ordinary differential equation (ODE) which can be written as:
which can be written as:
where
is the Legendre operator:
We use the Frobenius method to solve the equation in the region
. We start by setting the parameter p in Frobenius method zero.
,
,
.
Substituting these terms into the original equation, one obtains
-



![=\sum_{n=0}^{\infty}\left[-n(n-1)-2n+l(l+1)\right] a_n x^n
+ \sum_{n=0}^{\infty}n(n-1) a_n x^{n-2}](http://upload.wikimedia.org/math/6/1/9/6195b6fc880802f3fa1791ad9b72f34d.png)
![=\sum_{n=0}^{\infty}\left[l^2-n^2+l-n\right]a_n x^n
+ \sum_{n=-2}^{\infty}(n+2)(n+1) a_{n+2} x^n](http://upload.wikimedia.org/math/9/c/8/9c851890b232547f767ac6d0f63068ba.png)
.
Thus
,
and in general,
.
This series converges when
.
Therefore the series solution has to be cut by choosing:
.
The series cut in specific integers l and l+1 produce polynomials called Legendre polynomials.

![{d \over dx }[(1 - x^2){dy \over dx }]+l(l+1)y=0\,](http://upload.wikimedia.org/math/1/4/4/14477ff6b1b53099f191b05220388ee1.png)

![L={d \over dx }[(1 - x^2){d \over dx }]+l(l+1)\,](http://upload.wikimedia.org/math/3/2/0/3208f8f430c071be99a00bd6e01cb9b2.png)

