Series Solution of ODEs
Definition
The series solution method seeks a solution to an ODE as a power series
Intuition
If the ODE has analytic (variable) coefficients, its solutions are themselves analytic near an ordinary point, and can be written as convergent power series. Substituting the series into the ODE and matching powers of turns the differential equation into a recurrence relation on the coefficients — reducing “solve the ODE” to “find a pattern in the “. The two free constants and correspond to the two independent solutions guaranteed by linearity.
Formal Description
Differentiate term-by-term:
Substitute into the ODE and shift the summation index (e.g. in the sum) to align powers of :
Combine all sums into a single power series and set each coefficient to zero to obtain a recurrence relation for .
Example ():
Even and odd coefficients decouple, giving two independent sequences starting from and . The resulting series are recognised as
Key Results
- The method applies to ODEs with variable coefficients where closed-form solutions may be unavailable.
- Two independent series solutions arise from the two free constants and , in accordance with the principle of superposition.
- Convergence of the power series must be verified separately.
Applications
- Solving ODEs with polynomial coefficients near ordinary points (e.g.\ Legendre, Hermite, Chebyshev equations arising in physics).
- Deriving special functions (Bessel functions via Frobenius method at regular singular points).
- Verifying or discovering closed-form solutions for simple equations (as in the example above).
Trade-offs
- Only valid near ordinary points; singular points require the Frobenius method (series with a non-integer leading power).
- The radius of convergence is limited to the distance to the nearest singular point of the coefficients.
- Computing many terms of the recurrence is straightforward but can be tedious; closed-form recognition of the resulting series is not always possible.