method of integrating factors


The method of integrating factors is in principle a means for solving ordinary differential equationsMathworldPlanetmath of first .  It has not great practical significance, but is theoretically important.

Let us consider a differential equation solved for the derivativePlanetmathPlanetmath y′ of the unknown function and write the equation in the form

X⁢(x,y)⁢d⁢x+Y⁢(x,y)⁢d⁢y= 0. (1)

We assume that the functions X and Y have continuousMathworldPlanetmathPlanetmath partial derivativesMathworldPlanetmath in a region R of ℝ2.

If there is a solution of (1) which may be expressed in the form

f⁢(x,y)=C

with f having continuous partial derivatives in R and with C an arbitrary constant, then it’s not difficult to see that such an f satisfies the linear partial differential equation

X⁢∂⁡f∂⁡y-Y⁢∂⁡f∂⁡x= 0. (2)

Conversely, every non-constant solution f of (2) gives also a solution  f⁢(x,y)=C  of (1).  Thus, solving (1) and solving (2) are equivalentMathworldPlanetmathPlanetmathPlanetmathPlanetmathPlanetmath (http://planetmath.org/Equivalent3) tasks.

It’s straightforward to show that if  f0⁢(x,y)  is a non-constant solution of the equation (2), then all solutions of this equation are  F⁢(f0⁢(x,y))  where F is a freely chosen function with (mostly) continuous derivative.

The connection of the equations (1) and (2) may be presented also in another form.  Suppose that  f⁢(x,y)=C  is any solution of (1).  Then (2) implies the proportion equation

fx′X=fy′Y.

If we denote the common value of these two ratios by  μ⁢(x,y)=μ,  then we have

fx′=μ⁢X,fy′=μ⁢Y.

This gives to the differentialMathworldPlanetmath of the function f the expression

d⁢f⁢(x,y)=μ⁢(x,y)⁢(X⁢(x,y)⁢d⁢x+Y⁢(x,y)⁢d⁢y).

We see that  μ⁢(x,y)  is the integrating factor or Euler multiplicator of the given differential equation (1), i.e. the left hand side of (1) turns, when multiplied by  μ⁢(x,y),  to an exact differential (http://planetmath.org/ExactDifferentialForm).

Conversely, any integrating factor μ of (1), i.e. such that  μ⁢X⁢d⁢x+μ⁢Y⁢d⁢y  is the differential of some function f, is easily seen to determine the solutions of the form  f⁢(x,y)=C  of (1).  Altogether, solving the differential equation (1) is equivalent with finding an integrating factor of the equation.

When an integrating factor μ of (1) is available, the solution function f can be gotten from the line integral

f(x,y)=:∫P0P[μ(x,y)X(x,y)dx+μ(x,y)Y(x,y)dy]

along any curve γ connecting an arbitrarily chosen point  P0=(x0,y0)  and the point  P=(x,y)  in the region R.

Note.  In general, it’s very hard to find a suitable integrating factor.  One special case where such can be found, is that X and Y are homogeneous functions of same degree (http://planetmath.org/HomogeneousFunction): then the expression 1x⁢X+y⁢Y is an integrating factor.

Example.  In the differential equation

(x4+y4)⁢d⁢x-x⁢y3⁢d⁢y= 0

we see that  X=:x4+y4  and  Y=:-xy3  both define a homogeneous function of degree (http://planetmath.org/HomogeneousFunction) 4.  Thus we have the integrating factor  μ=:1x5+x⁢y4-x⁢y4=1x5,  and the left hand side of the equation

(1x+y4x5)⁢d⁢x-y3x4⁢d⁢y= 0

is an exact differential.  We can integrate it along the broken line, first from  (1, 0)  to  (x, 0)  and then still to  (x,y),  obtaining

f(x,y)=:∫1x(1x+04x5)dx-∫0yy3⁢d⁢yx4=ln|x|-y44⁢x4.

So the general solution of the given differential equation is

ln⁡|x|-y44⁢x4=C.

References

  • 1 E. Lindelöf: Differentiali- ja integralilasku III 1.  Mercatorin Kirjapaino Osakeyhtiö, Helsinki (1935).
Title method of integrating factors
Canonical name MethodOfIntegratingFactors
Date of creation 2013-03-22 16:31:48
Last modified on 2013-03-22 16:31:48
Owner pahio (2872)
Last modified by pahio (2872)
Numerical id 21
Author pahio (2872)
Entry type Topic
Classification msc 35-00
Classification msc 34-00
Related topic ErnstLindelof
Defines integrating factor
Defines Euler multiplicator