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A sound wave is essentially air particles oscillating parallel to the direction of travel of the wave.

We learnt that $v = f\lambda$, where $v$ is the speed of the wave, $f$ is the frequency of the wave and $\lambda$ is the wavelength of the wave.

Suppose the air particles oscillate with a frequency of $f_{particle}$. Is there any relationship between $f_{particle}$ and $v, f, \lambda$ of the entire sound wave?

I thought about this because intuitively, if the air particles vibrated faster, then the wave should travel faster, but I am unable to come up with any formula that describe this relationship (if it is even true!).

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  • $\begingroup$ How did you arrive at the idea, that the air particles should be oscillating with a different frequency than the wave itself? Why is that "intuitive"? $\endgroup$
    – CuriousOne
    Sep 18, 2014 at 9:45
  • $\begingroup$ In school the only thing we were ever taught about waves is to draw then as $\sin$ and $\cos$ curves. Sound waves were a $\sin$ curve, so were light waves and every other wave in our syllabus. If each point on the curve moved up and down faster, then the entire curve should travel faster, I think. $\endgroup$
    – Yiyuan Lee
    Sep 18, 2014 at 9:48
  • $\begingroup$ I see. Try this: imagine a wave on a lake. Imagine that there are leaves on the water that bob up and down with the wave. Are the leaves moving along with the wave, or are they standing still? What is the frequency of the movement of the leaves? Is it faster than the frequency of the wave, or the same? (If you don't have a lake and leaves, a sink and a bit of flower sprinkled on the water might do for an experiment!) $\endgroup$
    – CuriousOne
    Sep 18, 2014 at 9:54
  • $\begingroup$ Would that mean that the period of the individual particles is exactly the period of the wave? $\endgroup$
    – Yiyuan Lee
    Sep 18, 2014 at 9:55
  • $\begingroup$ Yep. If you don't believe me, you can do the experiment. By analogy, the same is true for sound waves, but it's harder to prove that experimentally, because the movement of air particles in a sound wave is much, much smaller (unless the volume of the sound is beyond deafening). $\endgroup$
    – CuriousOne
    Sep 18, 2014 at 9:57

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A sound wave is not particles oscillating, is a mechanical oscillation of a medium made of particles. It is important to separate the medium behaviour from the particle behaviour. Medium behaviour results from the averaging over the values of the many particles, and this generates essentially different phenomena.

A way of visualizing it is thinking of a demonstration or a public gathering: although many people are moving through, trying to reach a friend or coming out or in, the bulk behaviour is what matters if you would see from a plane. From above the mass would look static, even if below there is almost nobody standing in one place. The same is with movement, although not every person might move in the direction of the bulk, from above a marching crowd would look so. But the speeds and directions might differ very much.

So when sound travels through a medium, average densities oscillate due to pressure increase and vice versa. But local densities at a microscopic scale might me much larger than the bulk ones, because even if two particles can come very close, many of them cannot be so close together due to the much higher potential energy related.

So your analogy cannot be followed for these reasons, and this is also the cause that we use different formulations to describe groups of 10 or 100 particles, than when we describe media (made of at least ~$10^{23}$).

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