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We will now study a new class of differential equations similar to constant coefficient equations called Euler equations or Euler differential equations.

ax^{2} \cfrac{d^{2} y}{dx^{2} } +bx\cfrac{dy}{dx} +cy=0

This equation looks similar to the constant coefficient equation counterpart but there are some powers of x offsetting the derivatives. Recall the power rule.

{\cfrac{d}{dx} x^{n} =nx^{n-1}}
{\cfrac{d^{2} }{dx^{2} } x^{n} =n(n-1)x^{n-2} }

The factors of x in the variable coefficients build y back up to its original power in x if y is a power function. With this in mind we try a trial solution of

y=x^{\lambda }

{a\lambda (\lambda -1)x^{2} x^{\lambda -2} +b\lambda xx^{\lambda -1} +cx^{\lambda } =0}

{a\lambda (\lambda -1)x^{\lambda } +b\lambda x^{\lambda } +cx^{\lambda } =0}
(a\lambda^2+(b-a)\lambda+c)x^\lambda=0

This gives us an algebraic equation to solve instead of a differential equation like the characteristic equation for constant coefficient differential equations.

{a\lambda ^{2} +(b-a)\lambda +c=0}
{\lambda =-\cfrac{b-a}{2a} \pm \cfrac{\sqrt{(b-a)^{2} -4ac} }{2a}}
{\lambda =\lambda _{1} ,\lambda _{2} }

The general solution is therefore, at least when the roots are different,

y=c_{1} x^{\lambda _{1} } +c_{2} x^{\lambda _{2} }


Example 1. Find the solution to the following Euler equation

x^{2} \cfrac{d^{2} y}{dx^{2} } +x\cfrac{dy}{dx} -9y=0

Solution 1. We try a trial substitution of the form

y=cx^{\lambda }

This gives us an equation

 {\lambda (\lambda -1)+\lambda -9=0}
{\lambda =\pm 3}

The general solution is

y=c_{1} x^{3} +c_{2} x^{-3}

Curious as to what happens if the root repeats itself? Do we just multiply the solutions by another factor of x like we found for constant coefficients? It is likely not because we are not dealing with exponentials but power laws.


Example 2. Build a second order Euler equation with a repeated root and then solve it.
Solution 2. Well we need the discriminant to be zero so we have.

\lambda =-\cfrac{b-a}{2a} \pm \cfrac{\sqrt{(b-a)^{2} -4ac} }{2a}

We know that our repeated root will have a value of (a-b)/(2a), now we just have to pick the values such that

{(b-a)^{2} -4ac=0}
{{\rm Let:}\, c=1,\, a=1} \\ {(b-1)^{2} =4}
{b=1\pm 2=3,-1}

It doesn’t matter which we pick. Let us take b=3 then

x^{2} \cfrac{d^{2} y}{dx^{2} } +3x\cfrac{dy}{dx} +y=0

This equation has the repeated root of value

-\cfrac{b-a}{2a} =-\cfrac{3-1}{2} =-1

This would imply the solution would be

y=c_{1} x^{-1} +c_{2} x^{-1}

Since the order of the equation is two we expect two different solutions. We will try our trick to find the second one.

y=cu(x)x^{-1}

Substituting this into the original equation we find.

{x^{2} \cfrac{d^{2} }{dx^{2} } (ux^{-1} )+3x\cfrac{d}{dx} (ux^{-1} )+(ux^{-1} )=0}

{x^{2} \cfrac{d}{dx} (u'x^{-1} -ux^{-2} )+3x(u'x^{-1} -ux^{-2} )+ux^{-1} =0}
{x^{2} (u''x^{-1} -u'x^{-2} -u'x^{-2} +2ux^{-3} )+3x(u'x^{-1} -ux^{-2} )+ux^{-1} =0}

{u''x+u'(-1-1+3)+u(2x^{-1} -3x^{-1} +1x^{-1} )=0}

As a result of the differentiation we have a new differential equation of u to solve.

{xu''+u'=0}
{\cfrac{u''}{u'} =-\cfrac{1}{x} }
{\ln \left|u'\right|=-\ln \left|x\right|+C}
{\left|u'\right|=e^{-\ln \left|x\right|+C} =\cfrac{D}{x} }
{u(x)=A\ln \left|x\right|+B}

So our general solution turns out to be.

y=c_{1} x^{-1} +c_{2} x^{-1} \ln \left|x\right|

More advanced theory  shows that there is a factor of

(\ln \left|x\right|)^{n}

for every root repeated n times in higher order equations.


Example 3. If the Euler characteristic equation has roots

\lambda = a\pm ib

what does the form of the general solution look like?

Solution 3. We can use Euler’s formula to exponentiate a complex power function in terms of e rather than x.

x^{a+ib}=e^{(a+ib)\ln\left|x\right|}=x^a(\cos (b\ln\left|x\right|)+i\sin(b\ln\left|x\right|))

So the general solution will look like

y = x^a(A\cos (b\ln\left|x\right|)+B\sin(b\ln\left|x\right|))

when you combine both solutions.

Euler equations are a cute example of a type of differential equation that share many of the properties of constant coefficient differential equations, yet with their own twist. Remember which trial solution to use. Use

x^{\lambda }

for Euler equations, and use

e^{\lambda x}

for constant coefficient equations.

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Previous Topic: Nonhomogeneous Differential Equations

Next Topic: Differentiation with Respect to a Function


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