Legendre polynomials: Definition from Answers.com

Note: People sometimes refer to the more general associated Legendre polynomials as simply Legendre polynomials.

In mathematics, Legendre functions are solutions to Legendre's differential equation:

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

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 equation has regular singular points at x = ±1 so, in general, a series solution about the origin will only converge for |x| < 1. When n is an integer, the solution P_n(x) that is regular at x = 1 is also regular at x = −1, and the series for this solution terminates (i.e. is a polynomial).

These solutions for n = 0, 1, 2, ... (with the normalization P_n(1) = 1) 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:

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

The P_n are often defined as the coefficients in a Taylor series expansion:^[1]

$\frac{1}{\sqrt{1-2xt+t^2}} = \sum_{n=0}^\infty P_n(x) t^n\qquad (1)$ .

In physics, this generating function is the basis for multipole expansions.

1 Recursive Definition
2 The orthogonality property
3 Applications of Legendre polynomials in physics
4 Additional properties of Legendre polynomials
5 Shifted Legendre polynomials
6 Legendre polynomials of fractional order
7 See also
8 Notes
9 References
10 External links

Recursive Definition

Expanding the Taylor series in equation (1) for the first two terms gives

$P_0(x) = 1,\quad P_1(x) = x$

for the first two Legendre Polynomials. To obtain further terms without resorting to direct expansion of the Taylor series, equation (1) is differentiated with respect to t on both sides and rearranged to obtain

$\frac{x-t}{\sqrt{1-2xt+t^2}} = (1-2xt+t^2) \sum_{n=0}^\infty n P_n(x) t^{n-1}.$

Replacing the quotient of the square root with its definition in (1), and equating the coefficients of powers of t in the resulting expansion gives Bonnet’s recursion formula

$(n+1) P_{n+1}(x) = (2n+1) x P_n(x) - n P_{n-1}(x).\,$

This relation, along with the first two polynomials $P 0$ and $P 1$ , allows the Legendre Polynomials to be generated recursively.

The first few Legendre polynomials are:

n	$P_n(x)\,$
0	$1\,$
1	$x\,$
2	$\begin{matrix}\frac12\end{matrix} (3x^2-1) \,$
3	$\begin{matrix}\frac12\end{matrix} (5x^3-3x) \,$
4	$\begin{matrix}\frac18\end{matrix} (35x^4-30x^2+3)\,$
5	$\begin{matrix}\frac18\end{matrix} (63x^5-70x^3+15x)\,$
6	$\begin{matrix}\frac1{16}\end{matrix} (231x^6-315x^4+105x^2-5)\,$
7	$\begin{matrix}\frac1{16}\end{matrix} (429x^7-693x^5+315x^3-35x)\,$
8	$\begin{matrix}\frac1{128}\end{matrix} (6435x^8-12012x^6+6930x^4-1260x^2+35)\,$
9	$\begin{matrix}\frac1{128}\end{matrix} (12155x^9-25740x^7+18018x^5-4620x^3+315x)\,$
10	$\begin{matrix}\frac1{256}\end{matrix} (46189x^{10}-109395x^8+90090x^6-30030x^4+3465x^2-63)\,$

The graphs of these polynomials (up to n = 5) are shown below:

The orthogonality property

An important property of the Legendre polynomials is that they are orthogonal with respect to the L² inner product on the interval −1 ≤ x ≤ 1:

$\int_{-1}^{1} P_m(x) P_n(x)\,dx = {2 \over {2n + 1}} \delta_{mn}$

(where δ_mn denotes the Kronecker delta, equal to 1 if m = n and to 0 otherwise). In fact, an alternative derivation of the Legendre polynomials is by carrying out the Gram-Schmidt process on the polynomials {1, x, x², ...} with respect to this inner product. The reason for this orthogonality property is that the Legendre differential equation can be viewed as a Sturm–Liouville problem, and hence are eigenfunctions of a Hermitian differential operator:

${d \over dx} \left[ (1-x^2) {d \over dx} P(x) \right] = -\lambda P(x),$

where the eigenvalue λ corresponds to n(n + 1).

Applications of Legendre polynomials in physics

The Legendre polynomials were first introduced in 1782 by Adrien-Marie Legendre as the coefficients in the expansion of the Newtonian potential

$\frac{1}{\left| \mathbf{x}-\mathbf{x}^\prime \right|} = \frac{1}{\sqrt{r^2+r^{\prime 2}-2rr'\cos\gamma}} = \sum_{\ell=0}^{\infty} \frac{r^{\prime \ell}}{r^{\ell+1}} P_{\ell}(\cos \gamma)$

where $r$ and $r'$ are the lengths of the vectors $\mathbf{x}$ and $\mathbf{x}^\prime$ respectively and $γ$ is the angle between those two vectors. The series converges when $r > r'$ . The expression gives the gravitational potential associated to a point mass or the Coulomb potential associated to a point charge. The expansion using Legendre polynomials might be useful, for instance, when integrating this expression over a continuous mass or charge distribution.

Legendre polynomials occur in the solution of Laplace equation of the potential, $\nabla^2 \Phi(\mathbf{x})=0$ , in a charge-free region of space, using the method of separation of variables, where the boundary conditions have axial symmetry (no dependence on an azimuthal angle). Where $\widehat{\mathbf{z}}$ is the axis of symmetry and $θ$ is the angle between the position of the observer and the $\widehat{\mathbf{z}}$ axis (the zenith angle), the solution for the potential will be

$\Phi(r,\theta)=\sum_{\ell=0}^{\infty} \left[ A_\ell r^\ell + B_\ell r^{-(\ell+1)} \right] P_\ell(\cos\theta).$

$A_\ell$ and $B_\ell$ are to be determined according to the boundary condition of each problem^[2].

Legendre polynomials in multipole expansions

Figure 2

Legendre polynomials are also useful in expanding functions of the form (this is the same as before, written a little differently):

$\frac{1}{\sqrt{1 + \eta^{2} - 2\eta x}} = \sum_{k=0}^{\infty} \eta^{k} P_{k}(x)$

which arise naturally in multipole expansions. The left-hand side of the equation is the generating function for the Legendre polynomials.

As an example, the electric potential $Φ(r,θ)$ (in spherical coordinates) due to a point charge located on the z-axis at $z = a$ (Figure 2) varies like

$\Phi (r, \theta ) \propto \frac{1}{R} = \frac{1}{\sqrt{r^{2} + a^{2} - 2ar \cos\theta}}.$

If the radius r of the observation point P is greater than a, the potential may be expanded in the Legendre polynomials

$\Phi(r, \theta) \propto \frac{1}{r} \sum_{k=0}^{\infty} \left( \frac{a}{r} \right)^{k} P_{k}(\cos \theta)$

where we have defined η = a/r < 1 and x = cos θ. This expansion is used to develop the normal multipole expansion.

Conversely, if the radius r of the observation point P is smaller than a, the potential may still be expanded in the Legendre polynomials as above, but with a and r exchanged. This expansion is the basis of interior multipole expansion.

Additional properties of Legendre polynomials

Legendre polynomials are symmetric or antisymmetric, that is

$P_n(-x) = (-1)^n P_n(x). \,$ ^[1]

Since the differential equation and the orthogonality property are independent of scaling, the Legendre polynomials' definitions are "standardized" (sometimes called "normalization", but note that the actual norm is not unity) by being scaled so that

$P_k(1) = 1. \,$

The derivative at the end point is given by

$P_k'(1) = \frac{k(k+1)}{2}. \,$

As discussed above, the Legendre polynomials obey using the three term recurrence relation known as Bonnet’s recursion formula

$(n+1) P_{n+1}(x) = (2n+1) x P_n(x) - n P_{n-1}(x)\,$

and

${x^2-1 \over n} {d \over dx} P_n(x) = xP_n(x) - P_{n-1}(x).$

Useful for the integration of Legendre polynomials is

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

From Bonnet’s recursion formula one obtains by induction the explicit representation

$P_n(x) = \sum_{k=0}^n (-1)^k \begin{pmatrix} n \\ k \end{pmatrix}^2 \left( \frac{1+x}{2} \right)^{n-k} \left( \frac{1-x}{2} \right)^k.$

Shifted Legendre polynomials

The shifted Legendre polynomials are defined as $\tilde{P_n}(x) = P_n(2x-1)$ . Here the "shifting" function $x\mapsto 2x-1$ (in fact, it is an affine transformation) is chosen such that it bijectively maps the interval [0, 1] to the interval [−1, 1], implying that the polynomials $\tilde{P_n}(x)$ are orthogonal on [0, 1]:

$\int_{0}^{1} \tilde{P_m}(x) \tilde{P_n}(x)\,dx = {1 \over {2n + 1}} \delta_{mn}.$

An explicit expression for the shifted Legendre polynomials is given by

$\tilde{P_n}(x) = (-1)^n \sum_{k=0}^n {n \choose k} {n+k \choose k} (-x)^k.$

The analogue of Rodrigues' formula for the shifted Legendre polynomials is

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

The first few shifted Legendre polynomials are:

n	$\tilde{P_n}(x)$
0	1
1	$2 x - 1$
2	$6 x 2 - 6 x + 1$
3	$20 x 3 - 30 x 2 + 12 x - 1$

Legendre polynomials of fractional order

Legendre polynomials of fractional order exist and follow from insertion of fractional derivatives as defined by fractional calculus and non-integer factorials (defined by the gamma function) into the Rodrigues' formula. The exponents of course become fractional exponents which represent roots.

Notes

^ ^a ^b George B. Arfken, Hans J. Weber (2005). Mathematical Methods for Physicists. Elsevier Academic Press. p. 743. ISBN 0120598760.
^ Jackson, J.D. Classical Electrodynamics, 3rd edition, Wiley & Sons, 1999. page 103

References

Abramowitz, Milton; Stegun, Irene A., eds. (1965), "Chapter 8", Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables, New York: Dover, ISBN 0-486-61272-4, http://www.math.sfu.ca/~cbm/aands/page_332.htm See also chapter 22.
Bayin, S.S. (2006), Mathematical Methods in Science and Engineering, Wiley, Chapter 2.
Belousov, S. L. (1962), Tables of normalized associated Legendre polynomials, Mathematical tables series Vol. 18, Pergamon Press, 379 p.
Refaat El Attar (2009). Legendre Polynomials and Functions. CreateSpace. ISBN 978-1441490124.

External links

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