# Difference between a normal wave function and a standing-wave function

Nikitin
Hello! So as you all know the wave-function can be expressed as:

$$y(x,t) = A\cos(kx-\omega t)$$

However, this can be interpreted as both a standing and moving wave. So when do you interpret it as either of those? Are there any special conditions that should be written along with the wave function?

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How can this be interpreted as a standing wave?

Mentor
For the difference between traveling waves and standing waves, see e.g. here:

http://www.physics.buffalo.edu/claw/Page15/ProjectCLAW-P15.html [Broken]

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Nikitin
How can this be interpreted as a standing wave?

You could just use a identity to transform it into

$$A\cos(kx)\cos(\omega t)- A\sin(kx)\sin(\omega t)$$

Which is a sum of two clearly standing waves.

Am I wrong in saying that sum is a standing wave too? I have difficulties in graphing trig expressions in my mind.

jtbell: ahh, thanks I'll check it out now

Nikitin
OK after checking out jtbell's excellent website I see that I am an idiot for thinking that the wave function can be used to model a standing wave.

But still, what's up with a moving wave being the sum of two standing waves? Is this a random math-quirk or is there some physics behind this?

EDIT: Also, isn't it a bit weird that a standing-sound wave in a pipe open-ended on both sides is able to survive and stay standing for a long time? You'd think the two waves making up the standing wave would just dissipate out the ends the moment they reach them, but for some reason the waves get reflected back?

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Mentor
You could just use a identity to transform it into

$$A\cos(kx)\cos(\omega t)- A\sin(kx)\sin(\omega t)$$

Which is a sum of two clearly standing waves.

Yes, you can decompose a traveling wave into a sum of two standing waves. You can also decompose a standing wave into a sum of two traveling waves, which has a natural physical interpretation in terms of a single wave "bouncing back and forth" between the fixed ends of the string (or whatever the medium is).

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