Sometime in 2010 compiled on — Tuesday September 05, 2017 at 07:30 PM

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This note shows how to use the idea of eigenvalues and eigenfunctions to help guide finding a solution to a differential equation. There are many ways to solve this ODE, and this is a nicer more general way to looking at solving it.

Given

| (1) |

With some boundary conditions and

We start by rewriting this ODE as where is an operator applied on . This is just a rewrite of the ODE, we did not do anything new here, but this way it makes the equation look more like an , and this helps, for later when we discretize it and apply FDM (finite difference method), that what we will end up with. Also writing it as is more cool, and makes one look like a real math person.

Now that we have what to do? The whole point is to now find the eigenfunctions and eigenvalues of the operator (Recall, an operator has a matrix as a representation, is a mapping operator after all, so it is not far fetch to talk about an eigenvalues and eigenfunctions of an operator.).

Let us now call the eigenfunctions of as and the eigenvalues as .

So now we can write

But how to find these ? For the above ODE, it is done by inspection as it is clear that is an eigenfunction. We can see that because if we apply to it, we obtain

Hence it is now in the form , where , a scalar, and in this case

This is cool. We found the eigenfunctions and eigenvalues of Now what to do with them? Well, Since from (1) we see that is in the domain of the operator, because , and we just found the eigenfunctions of the operator, so then this is like saying that we found the basis vectors of the domain of where lives, and we need to use the basis vectors of this domain to represent . In other words,

| (2) |

The is just like in normal euclidean space, where we represent a vector as

The eigenfunctions are like the basis vectors and are like the coordinates of the vector . And is like the vector .

So far so good. We found the eigenfunctions of , and we rewrote in terms of these eigenfunctions. But wait a minute, we now have to find the . These are like the coordinates of when viewed in function space.

Here comes to the rescue something new that we need in order to make more progress. These eigenfunctions are not just some random things we pulled out of the sky. They are special functions and must adhere to some things. This is mathematics after all, and we must have some order.

These eigenfunctions must be orthogonal to each others and we define them on square integrable space We just made this restriction of the space to be able to make more headway in solving this problem.

What all this means, is that must be orthogonal to each others (just like are as a special case in the Euclidean space). Being in this space, we need to define an inner product on them. We need to know how to perform an inner product between and .

You might feel tricked now, because we did not say any of this stuff about the eigenfunctions when we found them above by inspection. But it is OK, luckily for us does meet these requirements. How? because if we define the inner product between and using

Then the above becomes

So, are orthogonal to each others. This is what orthogonal means. If we inner product any 2 different eigenfunctions with each others, we get zero, but if we inner product an eigenfunction with itself, we do not get zero.

Now we are really happy. We found that the eigenfunctions are orthogonal to each others, and we can express in term of them. We use this inner product property to find . We go back to (2) above, and multiply each side by and obtain

Integrating each side gives

But now we see that for and zero for all other terms so the above reduces to

Hence we just found

| (3) |

We take this and use it in (2). So, we have just found an expansion of in terms of the eigenfunctions . i.e. we have found a complete representation of as a function in the space of , with its basis vectors and the coordinates .

This is all so wonderful. But how does this help us to find the solution to well, if now just write , then we have

But hold a minute, this means that or

And this is the solution to the ode.

Hence given a differential operator , once we know its eigenfunctions and its eigenvalues, the problem is solved.

We just have to express the forcing function in terms of the eigenfunctions, and once this is done, the problem is solved. the solution is found. In real life, we obtain the matrix representation of , and we work on the matrix representation and find the eigenfunctions and eigenvalues. So, solving this ODE becomes a problem of finding eigenvalues and eigenfunctions. But remember, this all worked only because we were able to represent in terms of the eigenfunctions. If somehow we could not represent this way, then this whole approach falls apart.