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Power Series Solutions to the Legendre Equation
Power Series Solutions to the Legendre Equation
Department of Mathematics
IIT Guwahati
RA/RKS MA-102 (2016)
Power Series Solutions to the Legendre Equation
The Legendre equation
The equation
(1 −x2)y′′ −2xy′ +α(α+1)y = 0, (1)
where α is any real constant, is called Legendre’s equation.
+
When α ∈ Z , the equation has polynomial solutions called
Legendre polynomials. In fact, these are the same polynomial
that encountered earlier in connection with the Gram-Schmidt
process.
The Eqn. (1) can be rewritten as
2 ′ ′
[(x −1)y ] = α(α+1)y,
which has the form T(y) = λy, where T(f) = (pf′)′, with
p(x) = x2 −1 and λ = α(α+1).
RA/RKS MA-102 (2016)
Power Series Solutions to the Legendre Equation
Note that the nonzero solutions of (1) are eigenfunctions of T
corresponding to the eigenvalue α(α + 1).
Since p(1) = p(−1) = 0, T is symmetric with respect to the
inner product Z
1
(f , g) = f (x)g(x)dx.
−1
Thus, eigenfunctions belonging to distinct eigenvalues are
orthogonal.
RA/RKS MA-102 (2016)
Power Series Solutions to the Legendre Equation
Power series solution for the Legendre equation
The Legendre equation can be put in the form
y′′ + p(x)y′ + q(x)y = 0,
where
p(x) = − 2x and q(x) = α(α+1), if x2 6= 1.
1−x2 1−x2
Since 1 2 =P∞ x2n for |x| < 1, both p(x) and q(x) have
(1−x ) n=0
power series expansions in the open interval (−1,1).
Thus, seek a power series solution of the form
∞
y(x) = Xa xn, x ∈ (−1,1).
n
n=0
RA/RKS MA-102 (2016)
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