How to prove a wave is travelling ?

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Homework Help Overview

The discussion revolves around proving that a wave equation of the form f(x,t)=A•sin(k•x-ω•t) represents a traveling wave, with a focus on algebraic proof rather than graphical methods.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the nature of the wave as a fixed shape traveling in space and suggest setting the phase of the sine function to a constant to derive the location of points in the waveform over time. Others propose examining specific points on the wave, such as zeros, to deduce information about wave motion. There is also mention of the relationship between the wave equation and traveling waves, with emphasis on the conditions under which a wave retains its shape.

Discussion Status

The conversation is active with various participants offering insights and approaches to understanding the algebraic proof of the wave's traveling nature. Some guidance has been provided regarding the implications of the wave equation and the conditions for a wave traveling without changing shape.

Contextual Notes

Participants note the potential complexity of the topic, mentioning dispersion and the distinction between group velocity and phase velocity, which may affect the discussion of wave behavior.

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Homework Statement


This is not a homework of any form, I am simply interested in proving a wave equation of the form f(x,t)=A•sin(k•x-ω•t) is a traveling wave, preferably an algebraic proof. Thanks heaps!

Homework Equations


f(x,t)=A•sin(k•x-ω•t)

The Attempt at a Solution


I was able to proof this by using graphs, but I need to know the algebra behind it.
 
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Think of the wave as a 'waveform' (which is a fixed shape) that is traveling left or right.

Write an equation for the location of a particular point in the waveform, as a function of time.
A point in the waveform is uniquely determined by the argument to the sine function. So to fix the point in the waveform, set the phase equal to any constant C. So you have ##C=kx-\omega t##. Now solve for location ##x## as a function of ##t##. That tells you that the location of that point in the waveform is a linear function of time. It's easiest to visualise this if the point is a crest or a trough, where C is ##(2m+\frac12)\pi## or ##(2m-\frac12)\pi## respectively (##m## being an integer). But it's just as true for any point on the waveform.
 
Here's something to get you started. Look at the wave at a single point (for simplicity, look at a zero of the function). What can you deduce about the argument of the sine function? What does this tell you about the motion of the wave?

EDIT. Just got beat to it :frown:
 
To be a more accurate what you have here is a function ##f(x,t)## that satisfies the one dimensional wave equation https://en.wikipedia.org/wiki/Wave_equation

Any function that satisfies the wave equation is a traveling wave. (or in some cases a standing wave).

PS. You ll need to know a bit of differential calculus to understand the Wikipedia article.
 
Last edited:
i_hate_math said:

Homework Statement


This is not a homework of any form, I am simply interested in proving a wave equation of the form f(x,t)=A•sin(k•x-ω•t) is a traveling wave, preferably an algebraic proof. Thanks heaps!

Homework Equations


f(x,t)=A•sin(k•x-ω•t)

The Attempt at a Solution


I was able to proof this by using graphs, but I need to know the algebra behind it.
I guess we are talking about waves traveling without changing shape (otherwise we have to discuss dispersion, group velocity vs phase velocity, etc).

In general, if you have a function of the combination ##kx- \omega t## or of ##kx+ \omega t##, then you have a wave traveling to the right (or to the left in the second case) at a speed equal to ##v=\omega/k##. In other words, you can tell by using the following trick: if you set ##kx=\omega t## in the function and magically all dependence on x and t disappears, you have a wave traveling to the right without changing shape. If you set ##kx=-\omega t## in the function and magically all dependence on x and t disappears, you have a wave traveling to the left without changing shape.
 

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