The reason why steady packings of powders exist is precisely because
powders are athermal systems in the sense that their motion is not driven by thermal fluctuations (the particles are too big and too heavy to be bothered by thermal fluctuations)
powder grains have dissipative dynamics and can settle down into a mechanically equilibrated structure if one does regularly bring energy into the system (because they are big and heavy, their kinetic energy is sufficient to alter the cohesion of other particles during a collision...leading to elastic deformations dissipated in heat or plastic deformations of the particles or both)
For usual granular matter, the static properties such as achievable packing fractions and angle of repose are very much dependent on the protocol, the grain properties, its friction coefficient, its shape, the polydispersity, etc.
It depends so much on the protocol and details of the experiment that it has been reported that it also depends on temperature variations. In fact, since we have to deal with macroscopic grains, they can expand or contract because of temperature changes. In most packings with little friction, this can generate a loss of angle of repose momentarily until a new mechanical equilibrium is found.
Finally, I have to specify that in the case of the settlement of a powder on a substrate in absence of containing walls (context in which we can talk about angle of repose), if there is not enough friction between the grains and the substrate (if its surface is very very smooth or lubricated somehow), then the concept of angle of repose disappears and the powder literally "wets" the substrate as Aulo reported. Of course, contrary to the usual wetting of a molecular fluid, the cause here is more gravity than the van der Waals interaction between the grains and the substrate (although the latter does play some role too).
Now, for the simplest dynamical aspects, if one vibrates a powder very fast, it is possible to obtain a granular fluid regime that looks like a liquid or gas depending on the density. Despite all the efforts of the community on this topic it seems that for the specific reasons aforementioned it is impossible to get a one to one mapping between an actual fluid and a granular fluid although it is possible to rewrite most properties in a similar language. During avalanches, parts of the grains literally flow down a slope like a liquid but the velocity distribution is not Maxwellian for instance. Sand timers work on the same principle as water clocks (flowing down through a hole) but are more convenient than the latter because the flux of grains through the hole is independent of the height of the packing $h$ (contrary to most molecular fluids with a dependence on the $\sim \sqrt{h}$).
Finally, as it has been pointed out, granular flows can jam which is not the case for any molecular fluid that I know of (although this is a very controversial topic, the jamming transition has been shown to be quite distinct from the glass transition).
Now, your question is originally about downsizing the grains. That is possible up to few hundred microns at most. Below that scale, we reach the micron scale, and particles of that size are usually called colloids which refers to those particles that are neither molecules nor grains but in between. For that reason, they behave as real life toy model "molecules" once they are put in a solvent. This size dependent thermal regimes are discussed at the beginning of this paper although I have failed to retrieve the specific paper I have in mind on the subject.
In air, I am not really sure about how they behave, but most likely if you sweep some air, they will gain some altitude, attract one another via dispersion forces and can aggregate by doing so over long periods of time (that's how dust forms).
The two properties I have told about at the beginning (characteristic of powders) do not really hold anymore and the science of colloids consists then in trying to figure out how to pattern and treat these micron or sub-micron particles to make them interact in a way we like.
These colloidal systems have very rich phase behaviour including of course liquid-gas transition and fluid-solid transition among many others.