There are two regimes of operation for vacuum chambers, separated roughly by whether the “mean free path” for air molecules is short or long relative to the size of the chamber.
In the high-pressure limit, the mean free path is very short, and so the next thing any particular air molecule collides with is overwhelmingly likely to be another air molecule. I have in my head that a typical mean free path in air at atmospheric pressure is about sixty nanometers, but I haven’t taken the moment to confirm.
In this high-pressure limit, air acts like a fluid: it makes sense to talk about high- and low-pressure regions, and introducing a low-pressure region at the inlet of your vacuum pump will cause bulk airflow in the vacuum chamber. Information about pressure changes propagates through the fluid at roughly the speed of sound.
In the low-pressure limit, the mean free path is very long. Once the mean free path is much larger than your vacuum chamber, you no longer have pressure-driven bulk fluid flow: each air molecule is more likely to collide with the wall of the chamber than with another air molecule. In this regime, your pump no longer provides a pressure
gradient. Instead, the pump inlet is a region of the vacuum chamber wall where an air molecule is more likely to be removed from the vacuum volume than to scatter back in. This pressure-free density regime has a sensible name which I will suddenly remember in the shower tomorrow.
Airborne fine dust is a high-pressure phenomenon. The terminal velocity of a falling object is given by
$$
v_t= \sqrt\frac{2 m g}{\rho A C_d}
$$
for an object with weight $mg$, cross-section $A$, and drag coefficient $C_d$, falling in a fluid with density $\rho$. An “airborne” object is one whose terminal velocity is smaller than a typical air-current speed, so that random air currents may carry the object away from the ground. In the low-density $\rho\to 0$ limit, the terminal velocity is unbounded, because the drag responsible for the terminal-velocity approach becomes negligible.
As a commenter points out: if you like your vacuum chamber and your vacuum pumps, you should not put fine dust in them. Even if the dust is well-confined when you introduce it, accumulating in a neat pile because there are no air currents to blow it around: once you reintroduce air into the chamber, the dust will get everywhere.
How could activating the pump in a vacuum chamber not produce movement of the air inside? How could that not be the sole purpose of the pump?
However, loose powder is not air.
A "slow" pump might pass over any powder in a bowl…
A "fast" pump might suck the same powder first out of the bowl and into the chamber, then right out of the chamber.
– Robbie Goodwin Nov 08 '22 at 00:25