Wave on a string, and the chain rule argh

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Homework Help Overview

The discussion revolves around solving the wave equation using a change of variables, specifically with the substitutions \(\alpha = x + ct\) and \(\beta = x - ct\). The original poster is attempting to evaluate the second partial derivative of a function \(u\) with respect to \(x\) and is seeking clarification on the application of the chain rule in this context.

Discussion Character

  • Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • The original poster describes their attempts to apply the chain rule to find the second derivative and expresses confusion about the presence of mixed terms in the result. Some participants suggest considering the chain rule as an operator to facilitate the evaluation of derivatives.

Discussion Status

The discussion is active, with participants providing insights on how to approach the second derivative. The original poster acknowledges the suggestions and indicates that they found the input helpful in reframing their understanding of the problem.

Contextual Notes

The original poster mentions that they are reviewing the wave equation in preparation for graduate school, indicating a context of academic study and collaboration.

physmurf
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So, I am working through the wave equation for a review before my friend and I go off to grad school. It has been a couple of years since we both graduated with our BS in Physics.

So, here is the question:

Suppose I want to solve the wave equation using a change of variables. Let's use [tex]\alpha = x+ct[/tex], and [tex]\beta = x-ct, and\: u = \alpha + \beta[/tex]

The wave equation is
[tex]\frac{\partial^{2} u}{\partial t^{2}}=c^{2}\frac{\partial^{2} u}{\partial x^{2}}[/tex]


Now, if we take the partial derivative of u with respect to x and applying the chain rule one gets:

[tex]\frac{\partial u}{\partial x}=\frac{\partial u}{\partial \alpha}\frac{\partial \alpha}{\partial x}+\frac{\partial u}{\partial \beta}\frac{\partial \beta}{\partial x}[/tex]

Now if we evaluate [tex]\frac{\partial \alpha}{\partial x}, and \frac{\partial \beta}{\partial x}[/tex] we get
[tex]\frac{\partial u}{\partial x} = \frac{\partial u}{\partial \alpha} + \frac {\partial u}{\partial \beta}[/tex]

So, what and how do I evaluate the second partial differential with respect to x? I get

[tex]\frac{\partial^{2}u}{\partial x^{2}} = \frac{\partial^{2}u}{\partial \alpha^{2}}\ \frac{\partial \alpha}{\partial x}+\frac{\partial^{2}u}{\partial \beta^{2}}\ \frac{\partial \beta}{\partial x}[/tex]

Now, I know this isn't quite right. I am supposed to get:
[tex]\frac{\partial^{2}u}{\partial x^{2}} = \frac{\partial^{2}u}{\partial \alpha^{2}}\ \frac{\partial \alpha}{\partial x}+ \frac{\partial^{2}u}{\partial \alpha \partial \beta}}\ \frac{\partial \beta}{\partial x} + \frac{\partial^{2}u}{\partial \beta \partial \alpha}}\ \frac{\partial \alpha}{\partial x} +\frac{\partial^{2}u}{\partial \beta^{2}}\ \frac{\partial \beta}{\partial x}[/tex]

Can anyone help me? Thanks.
 
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just think about what d/dx is from your first chain rule equation (factor out the u on which the differential acts on). then use this to find the second derivative and u'll get the mixed terms.
 
When you are going for the second derivative, apply the operator:

[tex] \frac{\partial}{\partial x} = \frac{\partial \alpha}{\partial x} \frac{\partial}{\partial \alpha} + \frac{\partial \beta}{\partial x} \frac {\partial }{\partial \beta} [/tex]

to [tex]\frac{\partial u}{\partial x}[/tex].
 
Last edited:
Thanks for the input guys. That works. I just didn't think to look at it that way and treat the chain rule as an operator.
 

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