dunnoe said:
At first, I was skeptical that two periodic waves which are close in wavelength regardless of their shape will generate a beat frequency given only proof of the cosine-cosine case.
The reason you need only do the proof for the sinusoidal case is that every other periodic function can be expanded as a linear sum of sinusoids. Which is a separate proof.
Later, I toyed with MATLAB and plotted sine-sine, cosine-cosine & sine-squarewave graph which showed beat frequency as well. Surely there's a reason beyond geometry it's applicable for waves of all shapes .
Can you provide an example in math where there is a reason "beyond geometry" for something?
But you must realize that geometry is as basic as you can get.
eg. "Geometry, coeternal with God and shining in the divine Mind, gave God the pattern... by which he laid out the world so that it might be best and most beautiful and finally most like the Creator."
--- Johannes Kepler [1]
The effect you see is due to constructive and destructive interference - if the two waves have a different frequency then it follows that there must be a place where a trough of one must line up with a peak of the other and give you zero while at other places there must be two peaks or two troughs matching up and in-between you must get the, well, "in between" case.
What you are graphing is more: y=f(x).sin(kx) ... where f(x) happens to be another periodic with a different k. It doesn't have to be - all f(x) is doing is determining the amplitude of the sinusoid. Try f(x)=1/x for another famous example (you'll have to deal with what happens at x=0 though.).
You can also examine the case where the two waves have exactly the same frequency but different phases.
I don't think being able to derive a formula is the same as understanding the formula.
Well that's correct.
It's the trig ID that has you thrown off balance a bit?
It is a shortcut to actually doing the addition directly - with it's own separate proof.
One way of exploring underlying principles is to use the phasor representation for the waves - it's much more general.
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[1] Quoted by Field J. V. in:
Kepler's Geometrical Cosmology (1988), p. 123
quoted in Kepler's Geometrical Cosmology (1988), p. 123]