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 <title>Legendre polynomials</title>
 <name>LegendrePolynomials</name>
 <created>2006-05-22 23:05:06</created>
 <modified>2006-05-22 23:05:06</modified>
 <type>Definition</type>
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 <content>In mathematics, Legendre functions are solutions to Legendre's differential equation:

$$    {d \over dx} \left[ (1-x^2) {d \over dx} P(x) \right] + n(n+1)P(x) = 0.$$

They are named after Adrien-Marie Legendre. This ordinary differential equation is frequently encountered in physics and other technical fields. In particular, it occurs when solving Laplace's equation (and related partial differential equations) in spherical coordinates.

The Legendre differential equation may be solved using the standard power series method. The solution is finite (i.e. the series converges) provided $ |x| &lt; 1 $. Furthermore, it is finite at $x = ± 1$ provided n is a non-negative integer, i.e. $n = 0, 1, 2,...$ . In this case, the solutions form a polynomial sequence of orthogonal polynomials called the Legendre polynomials.

Each Legendre polynomial $P_n(x)$ is an nth-degree polynomial. It may be expressed using Rodrigues' formula:

 $$   P_n(x) = (2^n n!)^{-1} {d^n \over dx^n } \left[ (x^2 -1)^n \right]. $$

Not yet done.... derivative of wiki article</content>
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