What we are looking at in the simulation is a macroscopic simplification used to teach sound-wave mechanics.
In a real gas, the microscopic situation is much more chaotic. Air molecules are in constant, rapid, random thermal motion, even when no sound is present.
The Reality of Molecular Motion
Rapid thermal motion: At room temperature, air molecules typically move at speeds of several hundred meters per second, commonly around 450–500 m/s depending on the molecular species.
Frequent collisions: Individual molecules undergo enormous numbers of collisions with other molecules every second.
Mean free path: Between collisions, a molecule travels only a very small average distance—the mean free path, which in air at normal atmospheric conditions is on the order of tens of nanometers.
Therefore, an individual air molecule does not simply move back and forth around one fixed point as shown in the simulation.
Why We Use the Idealized Model
The simulation represents the air as small fluid elements or parcels rather than following individual molecules.
Average particle displacement
Although individual molecules move randomly, a sound wave produces a very small organized motion superimposed on this thermal motion.
The black dot in the simulation should therefore be understood as representing the average displacement of a small group of air molecules, or a fluid element, rather than the trajectory of one individual molecule.Visualizing wave propagation
If the true random thermal motion of every molecule were displayed, the organized acoustic motion would be almost impossible to see.
The simplified model removes this microscopic randomness so that we can clearly observe the coherent back-and-forth motion associated with the sound wave.Compression and rarefaction
Sound produces small variations in pressure and density.Compression: molecules are, on average, slightly closer together and pressure is higher.
Rarefaction: molecules are, on average, slightly farther apart and pressure is lower.
The equilibrium positions in the simulation provide a reference for displaying these small collective displacements.
Microscopic Reality vs. Acoustic Model
The simulation therefore does not represent the exact trajectories of individual air molecules.
It represents the macroscopic acoustic motion of the medium: the small, organized displacement of fluid elements superimposed on the much larger random thermal motion of individual molecules.
This illustrates the difference between:
Statistical mechanics — the microscopic, random motion of individual molecules
and
Continuum acoustics / wave mechanics — the organized pressure, density, and particle-displacement variations that constitute a sound wave.