Every nonhomogeneous differential equation has an associated homogeneous equation. The complementary solution is the solution to this homogeneous equation. It is an essential part of the general solution.
In simpler terms, the complementary solution solves the differential equation without considering the additional nonhomogeneous part (external forces). For the given differential equation:\[ x^{2} y'' - x y' - 3y = 0 \]the complementary solution can be represented as a combination of linearly independent solutions. Here, these solutions are given as:
- \(y_1 = \frac{1}{x}\)
- \(y_2 = x^3\)
A linear combination of these solutions (say, \(c_1y_1 + c_2y_2\) where \(c_1\) and \(c_2\) are constants) will form the complementary solution which is essential for the general solution. These solutions describe the behavior of the system in the absence of external forces.