Ordinary Differential Equations

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Homework Help Overview

The discussion revolves around finding eigenvalues and eigenfunctions for the ordinary differential equation -y''(x) = λy(x) with boundary conditions y(a) = y(b) = 0. The participants are exploring the implications of these conditions and the nature of the solutions.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the general form of the solutions, including the use of sine and cosine functions versus exponential functions. There is an exploration of how to apply boundary conditions to determine the eigenvalues and eigenfunctions.

Discussion Status

Some participants have provided insights into the general solution forms and the application of boundary conditions, while others are questioning the necessity of certain methods and seeking alternative approaches. There is a mix of interpretations regarding the general solution and its uniqueness.

Contextual Notes

Participants are considering the implications of the boundary conditions and the nature of the eigenvalues, with some expressing uncertainty about the general solution's form and its justification.

Combinatorics
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Homework Statement


Find all eigenvalues and eigenfunctions:
[itex]-y'' (x) = \lambda y(x) , x \in (a,b)[/itex]
[itex]y(a)= y(b) =0[/itex].


Homework Equations


[itex]sin x = \frac{e^{ix} + e^{-ix} }{2i}[/itex].

The Attempt at a Solution


So actually the only problem I have is to find the eigenfunctions (which should be something like [itex]sin \{ \frac{n \pi (x-a) }{(b-a)} \}[/itex] ) .
I received the eigenvalues are: [itex]\lambda_n = \frac{n^2 \pi^2 }{(b-a)^2}[/itex].
But how can I solve the two equations system I receive when applying these eigenvalues to the solution: [itex]y= c_1 e^{i \sqrt{\lambda_n} x} + c_2 e^{-i \sqrt{\lambda_n} x}[/itex].

I hope someone will be able to help me solve this two equations-system.

Thanks in advance!
 
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Combinatorics said:

Homework Statement


Find all eigenvalues and eigenfunctions:
[itex]-y'' (x) = \lambda y(x) , x \in (a,b)[/itex]
[itex]y(a)= y(b) =0[/itex].


Homework Equations


[itex]sin x = \frac{e^{ix} + e^{-ix} }{2i}[/itex].

The Attempt at a Solution


So actually the only problem I have is to find the eigenfunctions (which should be something like [itex]sin \{ \frac{n \pi (x-a) }{(b-a)} \}[/itex] ) .
I received the eigenvalues are: [itex]\lambda_n = \frac{n^2 \pi^2 }{(b-a)^2}[/itex].
But how can I solve the two equations system I receive when applying these eigenvalues to the solution: [itex]y= c_1 e^{i \sqrt{\lambda_n} x} + c_2 e^{-i \sqrt{\lambda_n} x}[/itex].

I hope someone will be able to help me solve this two equations-system.

Thanks in advance!

Write the problem as ##y'' +\lambda y = 0## and consider the case where ##\lambda = \mu^2 > 0## so ##y''+\mu^2y=0##. This gives you the solution pair ##\{e^{i\mu x},e^{-i\mu x}\}##. But by using appropriate linear combinations of those you could use the linearly independent pair ##\{\sin(\mu x),\cos(\mu x)\}## instead. Even better, you can use any appropriate linear combination of those to get something easier to work with. Try using this pair: ##\{\cos(\mu(x-a)),\sin(\mu(x-a))\}##. Take a general linear combination of those two and apply your boundary conditions. It will all drop out. At the end, remember ##\lambda = \mu^2.##
 
Is there any way of solving the two equations without having to do the process you mentioned?

Thanks !
 
One can, by direct substitution, show that [itex]y(x)= Acos(\lambda (x- a)+ Bsin(\lambda (x- a))[/itex] is the general solution to the differential equation [itex]y''+ \lambda^2 y= 0[/itex], for any number a. Of course, then [itex]y(0)= A= 0[/itex].
Now [itex]y(b)= B sin(\lambda(b- a))= 0[/itex]. You know, I presume that sin(x) is 0 if and only if x is a multiple of [itex]\pi[/itex] so you use that to determine possible values for the eigenvalue, [itex]\lambda[/itex].
 
Great ! Thanks ! But how can I prove that this is the general solution ? (i.e.- it obviously solves our problem...but why is it the general solution? why is it the only form of our eigenfunctions? )

Thanks!
 
Combinatorics said:
Is there any way of solving the two equations without having to do the process you mentioned?

Thanks !

I suppose so, but I don't know why you would want to. Certainly you would use ##y = A\cos(\mu x) + B\sin(\mu x)## instead of the exponential version. I will show you how to get the solution from there, assuming you didn't think of the ##(x-a)## version. Applying the boundary conditions you get:$$A\cos(\mu a) + B\sin(\mu a)=0$$ $$
A\cos(\mu b) + B\sin(\mu b)=0$$For this to have a non-trivial solution for ##A## and ##B## the determinant of coefficients must be 0:$$
\left |\begin{array}{cc}
\cos(\mu a) & \sin(\mu a)\\
\cos(\mu b) & \sin(\mu b)
\end{array}\right | =\cos(\mu a)\sin(\mu b)-\cos(\mu b)\sin(\mu a)= 0$$ $$
\sin(\mu(b-a))=0$$
This gives ##\mu(b-a) = n\pi## or ##\mu_n = \frac{n\pi}{b-a}##

Under this condition the system of equations is dependent, so just using the first one we can write ##A\cos(\mu a) = -B\sin(\mu a)## so ##A=-\frac{B\sin(\mu a)}{\cos(\mu a)}##. Substituting that for the ##A## in the general solution for ##y## gives $$
y_n = -B\frac{\sin(\mu_n a)}{\cos(\mu_n a)}\cos(\mu_n x) + B\sin(\mu_n x)
=(\frac{B}{\cos(\mu_n a)})(-\sin(\mu_n a)\cos(\mu_n x)+\sin(\mu_n x)\cos(\mu_n a))
=(\frac{B}{\cos(\mu_n a)})\sin(\mu_n(x-a))$$Since any constant times a solution is a solution, we can ignore the constant ##\frac{B}{\cos(\mu_n a)}## and take$$
y_n = \sin(\mu_n(x-a))$$So what I showed you in my first post is something worth learning. It saves a lot of work.
 
Last edited:
Thanks a lot !
 

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