Multivariable Calculus Chain Rule Problem: Wave equation

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Homework Help Overview

The discussion revolves around demonstrating that a specific function form is a solution to the wave equation in multivariable calculus. The function is expressed in terms of two variables, incorporating the wave speed parameter.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the implications of using different notations for derivatives and question the assumptions regarding the independence of variables in the context of the wave equation.

Discussion Status

Some participants have provided clarifications regarding the notation used for derivatives and the interpretation of functions of multiple variables. There is an acknowledgment of a misunderstanding about treating certain functions as dependent on multiple variables rather than separately.

Contextual Notes

Participants are navigating the nuances of notation in calculus, particularly in relation to partial derivatives and their implications for the wave equation. There is an emphasis on ensuring clarity in function definitions and variable independence.

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Homework Statement



Show that any function of the form

##z = f(x + at) + g(x - at)##

is a solution to the wave equation

##\frac {\partial^2 z} {\partial t^2} = a^2 \frac {\partial^2 z} {\partial x^2}##

[Hint: Let u = x + at, v = x - at]

2. The attempt at a solution

My problem with this is not that I haven't been able to solve it. The book's solution is right here:
hLVjQdS.png


I began to have trouble when I decided not to use f'(u) and g'(v) instead I used ##\frac {\partial z} {\partial u}## and ##\frac {\partial z} {\partial v}##

When I did this I got

##\frac {\partial^2 z} {\partial x^2} = \frac {\partial^2 z} {\partial u^2} + \frac {2 \partial^2 z } {\partial u \partial v} + \frac {\partial^2 z} {\partial v^2}##

and

##\frac {\partial^2 z} {\partial t^2} = a^2 (\frac {\partial^2 z} {\partial u^2} - \frac {2 \partial^2 z } {\partial u \partial v} + \frac {\partial^2 z} {\partial v^2})##

And that does not fulfill the condition stated in the beginning.

So I have a two questions in the end:

1)What is the difference between writing f'(u) and ##\frac {\partial z} {\partial u}##?

2)Do ##\frac {2 \partial^2 z } {\partial u \partial v}## and ##- \frac {2 \partial^2 z } {\partial u \partial v}## both evaluate to 0? (That's the only way ##\frac {\partial^2 z} {\partial t^2} = a^2 \frac {\partial^2 z} {\partial x^2}##) or did I do something wrong in my calculations?
 
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One ordinarily would use the notation f'(u) when f is deemed to be a function of a single variable, and ∂f/∂u when f is a function of several variables including u. However, the notation shouldn't make any difference.

Your problem is that when you went for ∂##^2##z/∂x##^2## you regarded ∂f/∂u as a function of both u and v, which it is not -- it is a function of u alone. Same with v. So you are not going to get any cross terms.

This may be a good reason why ∂f/∂u isn't a good way to notate f'(u).
 
Thank you so much. This has been bothering me for a while. So basically I interpreted this as ##f(u,v)## instead of ##f(u)## and ##g(v)## separately. Right?
 
Exactly right.
 

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