Annihilator method

In mathematics, the annihilator method is a procedure used to find a particular solution to certain types of non-homogeneous ordinary differential equations (ODEs).

[1] It is similar to the method of undetermined coefficients, but instead of guessing the particular solution in the method of undetermined coefficients, the particular solution is determined systematically in this technique.

The phrase undetermined coefficients can also be used to refer to the step in the annihilator method in which the coefficients are calculated.

The annihilator method is used as follows.

, find another differential operator

This operator is called the annihilator, hence the name of the method.

to both sides of the ODE gives a homogeneous ODE

for which we find a solution basis

Then the original inhomogeneous ODE is used to construct a system of equations restricting the coefficients of the linear combination to satisfy the ODE.

This method is not as general as variation of parameters in the sense that an annihilator does not always exist.

is in the natural numbers, and

are in the real numbers.

consists of the sum of the expressions given in the table, the annihilator is the product of the corresponding annihilators.

+ 5 y = sin ⁡ ( k x )

The simplest annihilator of

sin ⁡ ( k x )

, so the solution basis of

we find giving the system which has solutions giving the solution set This solution can be broken down into the homogeneous and nonhomogeneous parts.

) sin ⁡ ( k x )

is a particular integral for the nonhomogeneous differential equation, and

is a complementary solution to the corresponding homogeneous equation.

are determined usually through a set of initial conditions.

Since this is a second-order equation, two such conditions are necessary to determine these values.

The fundamental solutions

can be further rewritten using Euler's formula: Then

( cos ⁡ x + i sin ⁡ x ) +

( cos ⁡ x − i sin ⁡ x ) = (

sin ⁡ x

, and a suitable reassignment of the constants gives a simpler and more understandable form of the complementary solution,

sin ⁡ x )