In physical science and mathematics, Legendre polynomials (named after Adrien-Marie Legendre, who discovered them in 1782) are a system of complete and orthogonal polynomials, with a vast number of mathematically beautiful properties, and innumerable applications. They can be defined in many ways, and the various definitions highlight different aspects as well as suggest generalizations and connections to different mathematical structures and physical and numerical applications.
Closely related to the Legendre polynomials are Associated Legendre polynomials, Legendre functions of the second kind , discussed below, and associated Legendre functions. For each of these see the separate Wikipedia articles.
Definition by Construction as an Orthogonal SystemEdit
In this approach, the polynomials are defined as an orthogonal system with respect to the function over the interval , i.e., is a polynomial of degree , such that
This determines the polynomials completely up to an overall scale factor, which is fixed by the standardization . That this is a constructive definition is seen thus: is the only correctly standardized polynomial of degree 0. must be orthogonal to , leading to , is determined by demanding orthogonality to and , and so on. is fixed by demanding orthogonality to all with . This gives conditions, which, along with the standardization fixes all coefficients in . With work, all the coefficients of every polynomial can be systematically determined, leading to the explicit representation in powers of given below.
This definition of the 's is the simplest one. It does not appeal to the theory of differential equations. Second, the completeness of the polynomials follows immediately from the completeness of the powers 1, . Finally, by defining them via orthogonality with respect to the most obvious weight function on a finite interval, it sets up the Legendre polynomials as one of the three classical orthogonal polynomial systems. The other two are the Laguerre polynomials, which are orthogonal over the half line , and the Hermite polynomials, orthogonal over the full line , with weight functions that are the most natural analytic functions that ensure convergence of all integrals.
Definition via Generating FunctionEdit
The coefficient of is a polynomial in of degree . Expanding up to gives
Expansion to higher orders gets increasingly cumbersome, but is possible to do systematically, and again leads to one of the explicit forms given below.
It is possible to obtain the higher 's without resorting to direct expansion of the Taylor series, however. Eq. 2 is differentiated with respect to t on both sides and rearranged to obtain
This relation, along with the first two polynomials P0 and P1, allows all the rest to be generated recursively.
The generating function approach is directly connected to the multipole expansion in electrostatics, as explained below, and is how the polynomials were first defined by Legendre in 1782.
Definition via Differential EquationEdit
A third definition is in terms of solutions to Legendre's differential equation
This differential equation has regular singular points at x = ±1 so if a solution is sought using the standard Frobenius or power series method, a series about the origin will only converge for |x| < 1 in general. When n is an integer, the solution Pn(x) that is regular at x = 1 is also regular at x = −1, and the series for this solution terminates (i.e. it is a polynomial). The orthogonality and completeness of these solutions is best seen from the viewpoint of Sturm–Liouville theory. We rewrite the differential equation as an eigenvalue problem,
with the eigenvalue in lieu of . If we demand that the solution be regular at , the differential operator on the left is Hermitean. The eigenvalues are found to be of the form n(n + 1), with , and the eigenfunctions are the . The orthogonality and completeness of this set of solutions follows at once from the larger framework of Sturm-Liouville theory.
The differential equation admits another, non-polynomial solution, the Legendre functions of the second kind , discussed below. A two-parameter generalization of (Eq. 1) is called Legendre's general differential equation, solved by the Associated Legendre polynomials. Legendre functions are solutions of Legendre's differential equation (generalized or not) with non-integer parameters.
In physical settings, Legendre's differential equation arises naturally whenever one solves Laplace's equation (and related partial differential equations) by separation of variables in spherical coordinates. From this standpoint, the eigenfunctions of the angular part of the Laplacian operator are the spherical harmonics, of which the Legendre polynomials are (up to a multiplicative constant) the subset that is left invariant by rotations about the polar axis. The polynomials appear as where is the polar angle. This approach to the Legendre polynomials provides a deep connection to rotational symmetry. Many of their properties which are found laboriously through the methods of analysis --- for example the addition theorem --- are more easily found using the methods of symmetry and group theory, and acquire profound physical and geometrical meaning.
Orthonormality and CompletenessEdit
The standardization fixes the normalization of the Legendre polynomials (with respect to the L2 norm on the interval −1 ≤ x ≤ 1). Since they are also orthogonal with respect to the same norm, the two statements can be combined into the single equation,
That the polynomials are complete means the following. Given any piecewise continuous function with finitely many discontinuities in the interval [-1,1], the sequence of sums
converges in the mean to as , provided we take
This completeness property underlies all the expansions discussed in this article, and is often stated in the form
with −1 ≤ x ≤ 1 and −1 ≤ y ≤ 1.
Rodrigues' formula and other explicit formulasEdit
An especially compact expression for the Legendre polynomials is given by Rodrigues' formula:
This formula enables derivation of a large number of properties of the 's. Among these are explicit representations such as
where the last, which is also immediate from the recursion formula, expresses the Legendre polynomials by simple monomials and involves the multiplicative formula of the binomial coefficient.
The first few Legendre polynomials are:
The graphs of these polynomials (up to n = 5) are shown below:
Applications of Legendre polynomialsEdit
Expanding a 1/r potentialEdit
where r and r′ are the lengths of the vectors x and x′ 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's equation of the static potential, ∇2 Φ(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 ẑ is the axis of symmetry and θ is the angle between the position of the observer and the ẑ axis (the zenith angle), the solution for the potential will be
Al and Bl are to be determined according to the boundary condition of each problem.
They also appear when solving the Schrödinger equation in three dimensions for a central force.
Legendre polynomials in multipole expansionsEdit
Legendre polynomials are also useful in expanding functions of the form (this is the same as before, written a little differently):
If the radius r of the observation point P is greater than a, the potential may be expanded in the Legendre polynomials
where we have defined η = a/ < 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.
Legendre polynomials in trigonometryEdit
The trigonometric functions cos nθ, also denoted as the Chebyshev polynomials Tn(cos θ) ≡ cos nθ, can also be multipole expanded by the Legendre polynomials Pn(cos θ). The first several orders are as follows:
Another property is the expression for sin (n + 1)θ, which is
Additional properties of Legendre polynomialsEdit
Another useful property is
- for ,
which follows from considering the orthogonality relation with . It is convenient when a Legendre series is used to approximate a function or experimental data: the average of the series over the interval [-1, 1] is simply given by the leading expansion coefficient .
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 1) by being scaled so that
The derivative at the end point is given by
The Askey–Gasper inequality for Legendre polynomials reads
where the unit vectors r and r′ have spherical coordinates (θ,φ) and (θ′,φ′), respectively.
As discussed above, the Legendre polynomials obey the three-term recurrence relation known as Bonnet’s recursion formula
Useful for the integration of Legendre polynomials is
From the above one can see also that
where ||Pn|| is the norm over the interval −1 ≤ x ≤ 1
Asymptotically for l → ∞
and for arguments of magnitude greater than 1
where J0 and I0 are Bessel functions.
All zeros of are real, distinct from each other, and lie in the interval . Further, if we regard them as dividing the interval into subintervals, each subinterval will contain exactly one zero of . This is known as the interlacing property. Because of the parity property it is evident that if is a zero of , so is . These zeros play an important role in numerical integration based on Gaussian quadrature. The specific quadrature based on the 's is known as Gauss-Legendre quadrature.
Legendre polynomials with transformed argumentEdit
Shifted Legendre polynomialsEdit
The shifted Legendre polynomials are defined as
An explicit expression for the shifted Legendre polynomials is given by
The analogue of Rodrigues' formula for the shifted Legendre polynomials is
The first few shifted Legendre polynomials are:
Legendre rational functionsEdit
A rational Legendre function of degree n is defined as:
Legendre functions of the second kind (Qn)Edit
As well as polynomial solutions, the Legendre equation has non-polynomial solutions represented by infinite series. These are the Legendre functions of the second kind, denoted by Qn(x).
The differential equation
has the general solution
where A and B are constants.
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|Wikimedia Commons has media related to Legendre polynomials.|
- A quick informal derivation of the Legendre polynomial in the context of the quantum mechanics of hydrogen
- Hazewinkel, Michiel, ed. (2001) , "Legendre polynomials", Encyclopedia of Mathematics, Springer Science+Business Media B.V. / Kluwer Academic Publishers, ISBN 978-1-55608-010-4
- Wolfram MathWorld entry on Legendre polynomials
- Dr James B. Calvert's article on Legendre polynomials from his personal collection of mathematics
- The Legendre Polynomials by Carlyle E. Moore
- Legendre Polynomials from Hyperphysics