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 <title>Legendre polynomials</title>
 <name>LegendrePolynomials</name>
 <created>2006-05-22 23:05:06</created>
 <modified>2006-05-24 04:46:53</modified>
 <type>Definition</type>
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 <content>The Legendre polynomials generate the power series that solves Legendre's differential equation:

$$   \left ( 1 - x^2 \right ) P''(x) - 2x P'(x) + n(n+1)P(x) = 0.$$

This ordinary differential equation with variable coefficients is named in honor of Adrien-Marie Legendre (1752-1833).  While quite literally following in the footsteps of Laplace, he developed the Legendre polynomials in a paper on celestial mechanics.  In a strange tangled web of fate, the Legendre polynomials are heavily used in electrostatics to solve Laplace's equation in spherical coordinates

$$ \nabla^2 \Phi_{sph} = 0 $$

Not yet done.... below is derivative of wiki article

. 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:

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



\subsection{References}

http://www-groups.dcs.st-and.ac.uk/~history/Biographies/Legendre.html
http://astrowww.phys.uvic.ca/~tatum/celmechs.html</content>
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