Wave on a string, and the chain rule argh

[physmurf]

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 \alpha = x+ct, and \beta = x-ct, and\: u = \alpha + \beta

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


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

\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}

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

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

\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}

Now, I know this isn't quite right. I am supposed to get:
\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}

Can anyone help me? Thanks.

 

[Gianni2k]

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.

 

[Dick]

When you are going for the second derivative, apply the operator:

<br /> \frac{\partial}{\partial x} = \frac{\partial \alpha}{\partial x} \frac{\partial}{\partial \alpha} + \frac{\partial \beta}{\partial x} \frac {\partial }{\partial \beta} <br />

to \frac{\partial u}{\partial x}.

 

[physmurf]

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.