Reduction of order

Summary

Reduction of order (or d’Alembert reduction) is a technique in mathematics for solving second-order linear ordinary differential equations. It is employed when one solution is known and a second linearly independent solution is desired. The method also applies to n-th order equations. In this case the ansatz will yield an (n−1)-th order equation for .

Second-order linear ordinary differential equations edit

An example edit

Consider the general, homogeneous, second-order linear constant coefficient ordinary differential equation. (ODE)

 
where   are real non-zero coefficients. Two linearly independent solutions for this ODE can be straightforwardly found using characteristic equations except for the case when the discriminant,  , vanishes. In this case,
 
from which only one solution,
 
can be found using its characteristic equation.

The method of reduction of order is used to obtain a second linearly independent solution to this differential equation using our one known solution. To find a second solution we take as a guess

 
where   is an unknown function to be determined. Since   must satisfy the original ODE, we substitute it back in to get
 
Rearranging this equation in terms of the derivatives of   we get
 

Since we know that   is a solution to the original problem, the coefficient of the last term is equal to zero. Furthermore, substituting   into the second term's coefficient yields (for that coefficient)

 

Therefore, we are left with

 

Since   is assumed non-zero and   is an exponential function (and thus always non-zero), we have

 

This can be integrated twice to yield

 
where   are constants of integration. We now can write our second solution as
 

Since the second term in   is a scalar multiple of the first solution (and thus linearly dependent) we can drop that term, yielding a final solution of

 

Finally, we can prove that the second solution   found via this method is linearly independent of the first solution by calculating the Wronskian

 

Thus   is the second linearly independent solution we were looking for.

General method edit

Given the general non-homogeneous linear differential equation

 
and a single solution   of the homogeneous equation [ ], let us try a solution of the full non-homogeneous equation in the form:
 
where   is an arbitrary function. Thus
 
and
 

If these are substituted for  ,  , and   in the differential equation, then

 

Since   is a solution of the original homogeneous differential equation,  , so we can reduce to

 
which is a first-order differential equation for   (reduction of order). Divide by  , obtaining
 

The integrating factor is  .

Multiplying the differential equation by the integrating factor  , the equation for   can be reduced to

 

After integrating the last equation,   is found, containing one constant of integration. Then, integrate   to find the full solution of the original non-homogeneous second-order equation, exhibiting two constants of integration as it should:

 

See also edit

References edit

  • Boyce, William E.; DiPrima, Richard C. (2005). Elementary Differential Equations and Boundary Value Problems (8th ed.). Hoboken, NJ: John Wiley & Sons, Inc. ISBN 978-0-471-43338-5.
  • Teschl, Gerald (2012). Ordinary Differential Equations and Dynamical Systems. Providence: American Mathematical Society. ISBN 978-0-8218-8328-0.
  • Eric W. Weisstein, Second-Order Ordinary Differential Equation Second Solution, From MathWorld—A Wolfram Web Resource.