Sturm-Liouville Orthogonality Proof

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Homework Help Overview

The discussion revolves around the Sturm-Liouville equation and the orthogonality of derivatives of eigenfunctions. The original poster is tasked with demonstrating that the derivatives of a set of eigenfunctions are also orthogonal and determining the appropriate weighting function and boundary conditions for this orthogonality.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • The original poster questions the meaning of orthogonality for the derivatives and whether it implies a specific integral relationship. They express confusion about how the boundary conditions relate to the problem.
  • Some participants suggest that the derivatives may form their own Sturm-Liouville problem and explore the existence of a weighting function.
  • Others discuss methods for showing orthogonality by manipulating the Sturm-Liouville equation and integrating, while questioning the validity of their approaches and the need for explicit expressions for the weighting function.

Discussion Status

The discussion is active, with participants exploring various interpretations and methods for demonstrating orthogonality. Some have proposed potential approaches and boundary conditions, while others express uncertainty about their reasoning and seek clarification on specific steps.

Contextual Notes

Participants are navigating the implications of boundary conditions and the requirements for orthogonality in the context of Sturm-Liouville theory. There is an acknowledgment of the need for a weighting function, but its exact form remains under discussion.

Conor_McF
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Homework Statement



A set of eigenfunctions yn(x) satisfies the Sturm-Liouville equation #1 with boundary conditions #2. The function g(x) = 0. Show that the derivatives un(x) = yn'(x) are also orthogonal functions. Determine the weighting function w(x) for these functions. What boundary conditions are required for orthogonality?

Homework Equations



#1: [tex]\frac{d}{dx}[/tex]f(x)[tex]\frac{dy}{dx}[/tex] - g(x)[tex]\frac{dy}{dx}[/tex] + [tex]\lambda[/tex]w(x)y = 0 where w(x) [tex]\geq[/tex] 0 and a [tex]\leq[/tex] x [tex]\leq[/tex] b

#2: [tex]\alpha[/tex]1y + [tex]\beta[/tex]1[tex]\frac{dy}{dx}[/tex] = 0 at x = a and [tex]\alpha[/tex]2y + [tex]\beta[/tex]2[tex]\frac{dy}{dx}[/tex] = 0 at x = b

[tex]\alpha[/tex] and [tex]\beta[/tex] are both constants and cannot both equal 0.

There is also the orthogonality relation [tex]\int y_{n}w(x)y_{m}dx = 0[/tex]


The Attempt at a Solution



I guess what I'm most confused about here is what the problem is asking me to show. By saying the set "un(x) = yn'(x) are orthogonal functions", what exactly are they orthogonal to? I'm assuming it means that [tex]\int u_{n}w(x)u_{m}dx = 0[/tex], provided that m [tex]\neq[/tex] n. Is this correct or am I way off?

Since g(x) = 0, the DE becomes [tex]\frac{d}{dx}[/tex]f(x)[tex]\frac{dy}{dx}[/tex] + [tex]\lambda[/tex]w(x)y = 0. From the boundary conditions I can tell that y(a) = - [tex]\frac{\alpha_{1}}{\beta_{1}}[/tex]u(a) and y(b) = - [tex]\frac{\alpha_{2}}{\beta_{2}}[/tex]u(b), but I don't know how this would help me at all. Can somebody please point me in the right direction?

Thanks; Conor.
 
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might be on the wrong track, but here's a guess...

based on the wording of the question i think you need to show the u's are orthogonal, as you've written, but to some weighting function yet to be determined

how about trying to show the u's constitute their own sturm-liouville problem? existence and orthogonality properties of the solutions would show the un are orthogonal?

did this and got a weighting function ~(d/dx(f'/w)+lambda)... though not sure how to show this is >0 for all x...
 
Yeah, that's what I thought to, but how did you show that they form their own Sturm-Liouville problem? Did you replace y(x) with u(x) in #1? When you sub the u(x)'s into eq'n #1, the last term contains [tex]\int u(x)dx[/tex], because u = y'. I'm curious to see how you got that weighting function.

I did it a little differently, but I'm not sure if I'm cheating. If you take eqn #1 in both n and m (two different indicies), multiply both by ym and ym (respectively), add the two equations and then integrate over all x you get...

[tex]\int\left[y_{m}\frac{d}{dx}f\frac{dy_{n}}{dx} + y_{n}\frac{d}{dx}f\frac{dy_{m}}{dx}\right]dx = - \left( \lambda_{n} - \lambda_{m} \right) \int y_{n}w(x)y_{m}dx = 0[/tex] (because of orthogonality of y)​

It turns out that the first and second terms in the integration are equal due to symmetry in m and n, making the integral equal to...

[tex]2\left(\frac{\beta_{1}}{\alpha_{1}}u_{n}(a)f(a)u_{m}(a) - \frac{\beta_{2}}{\alpha_{2}}u_{n}(b)f(b)u_{m}(b)\right) - 2\int u_{n}f(x)u_{m}dx = 0[/tex]​

...where I've made use of the boundary conditions and integration by parts. The additional boundary condition the problem is asking for in this case could be...

[tex]\frac{\beta_{1}}{\alpha_{1}}u_{n}(a)f(a)u_{m}(a) = \frac{\beta_{2}}{\alpha_{2}}u_{n}(b)f(b)u_{m}(b)[/tex]​

...in which case [tex]\int u_{n}f(x)u_{m}dx = 0[/tex] and the [tex]u_{n}[/tex] are orthogonal, and f(x) is the weighting function. I am concerned, however, that I did not obtain an actual expression for f(x), as the problem may have been asking. If you have time, please show me how you got your weighting function. Thanks for your help!
 
nice idea,

don't even need to add the 2 equations, Also i would try and write the boundary conditions independent of m,n maybe this could be done by

y'(a) = [tex]\sqrt{f(a)\beta 1 \alpha 2 / (f(b)\beta 2 \alpha 1)[/tex] y'(b)


not convinced with what i did now as i don't think its in correct SL form

but method was
- sub in u =y'
- divide by w & then differentiate
- try to re-arrange into SL form
 
Yeah good call, I guess you don't need to add them. I'll try to rewrite those boundary conditions.
 

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