Variation of Parameters and the Wronskian
1Introduction
This lecture develops variation of parameters, which constructs a particular solution of a nonhomogeneous equation from a fundamental pair of homogeneous solutions. It formulates nonvanishing of the Wronskian as an interval-wide condition and explains the role of constants of integration.
2Hypotheses and a Fundamental Pair
On an interval , consider
where are continuous on . Let be a fundamental pair for the corresponding homogeneous equation; that is, they are linearly independent solutions on .
Define the {Wronskian} by
Abel's identity states that
Thus, if at one point of , then throughout . Conversely, vanishing at one point implies vanishing throughout the interval. For a homogeneous equation with continuous coefficients, nonvanishing need not be assumed separately at every point.
3Derivation of Variation of Parameters
Set
and impose
Then . Differentiating once more and substituting into the original equation leaves
Therefore,
Since on , Cramer's rule gives
4Definite-Integral Formula
Fix a base point . Then
so a particular solution is
This choice satisfies . If indefinite integrals are used instead, their arbitrary constants contribute and are absorbed into the homogeneous solution. Hence the general solution is
5Example:
Fix any interval on which is continuous,
The functions and form a fundamental pair on , with . Thus,
One choice of antiderivatives is
The cross terms cancel in , yielding
This expression is defined on the selected interval , and direct substitution verifies . Different integration constants merely add a homogeneous solution.
6Method Selection and Limitations
Undetermined coefficients has lower computational cost when its hypotheses hold. Variation of parameters is less dependent on the form of , but a fundamental pair must already be known, and the resulting integrals need not be elementary. The method must be applied separately on each interval where are simultaneously continuous.
An analogous formula using a fundamental matrix exists for first-order linear systems. Its details are deferred to the subsequent lectures on systems.