Legendre polynomials: Difference between revisions
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:<math>x^6= \frac{1}{231}[33P_0 (x) + 110P_2(x)+ 72P_4(x)+ 16P_6(x)]</math> | :<math>x^6= \frac{1}{231}[33P_0 (x) + 110P_2(x)+ 72P_4(x)+ 16P_6(x)]</math> | ||
==Applications in statistical mechanics== | |||
*[[Computational implementation of integral equations]] | |||
*[[Order parameters]] | |||
*[[Lebwohl-Lasher model]] | |||
*[[Rotational relaxation]] | |||
==See also== | ==See also== | ||
*[[Associated Legendre function]] | *[[Associated Legendre function]] |
Latest revision as of 11:06, 7 July 2008
Legendre polynomials (also known as Legendre functions of the first kind, Legendre coefficients, or zonal harmonics) are solutions of the Legendre differential equation. The Legendre polynomial, can be defined by the contour integral
Legendre polynomials can also be defined (Ref 1) using Rodrigues formula, used for producing a series of orthogonal polynomials, as:
Legendre polynomials form an orthogonal system in the range [-1:1], i.e.:
- for
whereas
The first seven Legendre polynomials are:
"shifted" Legendre polynomials (which obey the orthogonality relationship in the range [0:1]):
Powers in terms of Legendre polynomials:
Applications in statistical mechanics[edit]
- Computational implementation of integral equations
- Order parameters
- Lebwohl-Lasher model
- Rotational relaxation
See also[edit]
References[edit]
- B. P. Demidotwitsch, I. A. Maron, and E. S. Schuwalowa, "Métodos numéricos de Análisis", Ed. Paraninfo, Madrid (1980) (translated from Russian text)