I saw this unintuitive result on dice packing:

A jumble of thousands of cubic dice, agitated by an oscillating rotation, can rapidly become completely ordered, a result that is hard to produce with more conventional shaking.

The paper is not very rigorous.

  1. Is there a mathematical explanation of this result?

  2. Is such phenomenon studied?

Can the presence of centripetal force in oscillating rotation help explain the phenomenon?

Update: Why does entropy seemingly reduce? Is there information theoretic explanation?

K. Asencio et al., Phys. Rev. Lett. (2017)

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    $\begingroup$ Maybe, the complete order is a stable fixed point for the rotation, but is not for a shaking? $\endgroup$ – Fedor Petrov Dec 16 '17 at 22:06
  • $\begingroup$ @FedorPetrov Interesting idea. $\endgroup$ – 1.. Dec 16 '17 at 22:36
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    $\begingroup$ This is an extraordinarily interesting phenomenon and it certainly makes a nice question both in the mathematical and physical level! I have not yet find time to read the paper carefully but i cannot help myself from thinking that it is strongly reminiscent of the Ising model of ferromagnetism; in the sense that it includes "nearest neighbor interactions" and displays some kind of "phase transition". $\endgroup$ – Konstantinos Kanakoglou Dec 17 '17 at 5:26
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    $\begingroup$ Top down video at physics.aps.org/articles/v10/130 apparently demonstrating a threshold angular acceleration for dice nearer the centre to become aligned $\endgroup$ – Henry Dec 17 '17 at 23:49
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    $\begingroup$ They are cubes not dice, their "dicenesss" and printed numbers are irrelevant 100% so I suggest taking away this confounding factor in the title that makes the question harder to find. $\endgroup$ – Santropedro Dec 18 '17 at 2:47

• Concerning question 2, you might want to take a look at Simulation of cubical particle packing under mechanical vibration (2016). The precise effect mentioned in the 2017 paper is not considered in that study, but a variety of ordering mechanisms are examined.

• Concerning question 1, the complexity of this mechanical problem (in the sense of many competing mechanisms) does not lend itself to a clear-cut mathematical formulation; all progress I am aware of is closely tied to either experiments or computer simulations of the ordering process.

All of this is in contrast to the order-disorder transition in thermal equilibrium, which does lend itself to a purely mathematical treatment (given the Hamiltonian, calculate the partition function). Here we are far from equilibrium, and then there are too many competing effects for a compact and precise mathematical formulation.

• Concerning the question added in the 2019 update: Locally, entropy may decrease if it is balanced by an increase in entropy in the surroundings. In the experiment the ordering does not happen in the isolated system, it is driven by the externally induced mechanical vibration, which will produce the entropy needed to offset the entropy loss. This happens in any phase transition, think of placing a glass of water in the freezer.

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    $\begingroup$ The authors use buzz words - entropy, statistical mechanics - may be there is a mathematical technique. $\endgroup$ – 1.. Dec 16 '17 at 16:49

I doubt that a mathematically rigorous explanation of the phenomenon discovered in that paper exists using today's technology. While mathematical statistical mechanics is a well-developed field of study, there is still much to be done before the applications of statistical mechanics by physicists can be made rigorous.

Any explanation should include a mathematical description of the "before-shaking" and "after-shaking" configurations; this should include a rigorous definition as well as a proof of some of their basic properties.

The "after-shaking" configuration seems to be related to the usual close-packing of cubes, where the cubes are congruent to a configuration where their centers are on $\mathbb{Z}^3$. (Understanding how this relates to what is seen with the cylindrical boundary conditions seems hard though). The "before-shaking" configuration then seems to correspond to a "disordered jammed" packing of the cubes. So far as I know, the set of such packings is not understood mathematically (though I would be delighted to be proven wrong!).

Let me explain this a bit more. Let $\mathcal{C}_{N,L}$ be the configuration space of $N$ hard cubes in a periodic box of size $L\times L\times L$; this is a semialgebraic subset of the $6N$-dimensional space of all possible positions and orientations. One can discuss jamming of configurations in terms of the connected components of the family of these spaces as $L$ changes (see e.g. this old mathoverflow question on the configuration space of hard disks).

For $N$ small enough, presumably one can show that there are often jammed configurations of cubes which do not come from the close-packed cubic lattice state. However, we are really interested in the thermodynamic limit where $N,L\rightarrow\infty$ with the density $N/L^3$ fixed and so far as I know, no one has been able to say anything about the ensemble of these jammed configurations in that limit; for example, it would be nice to have a proof that there exists a disordered thermodynamic phase of jammed configurations.

Even in the absence of proof, we still have some idea of what happens as one changes the density (an understanding at the level of physics, not mathematics). See for example my old answer here for references to experimental and simulation work on packed cubes and some more discussion about jamming.

Anyways, here's the punchline:

We've run into all of these difficulties (even in the world of equilibrium statistical mechanics) and we haven't even discussed the real meat of the paper: the driven, dissipative dynamics of these hard cubes in the presence of gravity and curved boundary conditions and friction!

P.S. I doubt this was your intention, but saying without any qualification that an experimental paper "is not very rigorous" would ordinarily be interpreted as saying that the design of the experiments or the way they were carried out was sloppy. That is not my understanding from reading the paper.

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The physical reason is that the cubically packed state has lower gravitational potential energy than the jammed random state. The overall process is analogous to annealing, although the reduction in energy in the latter case is to do with atomic bonding, not gravity.

For the process to work, it is necessary for the jostling to be enough to ease the elements (dice in this case) out of their unstable or metastable positions so that they can fall into stable lower-energy aligned positions, but not so violent that they are thrown back out of these lower positions.

The cubically packed state is obviously of maximum density; so the centre of gravity is the lowest among all possible configurations.

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    $\begingroup$ Energy is one ingredient in the order-disorder transition, but entropy is another. The cited paper argues that the walls of the container prefer an ordered layer perpendicular to the boundaries, and this mechanism would work even in the absence of gravity. $\endgroup$ – Carlo Beenakker Dec 16 '17 at 21:58
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    $\begingroup$ @CarloBeenakker: If the elements are many, so that the proportion of them adjacent to the container is small, then the contribution of the peripheral elements to the lowering of the centre of gravity is marginal. If the position of the peripheral elements is nevertheless considered, and the container walls are flat or only gently curved, then maximal density is achieved when the elements are aligned as close as possible to the wall, which is the case when the vertical faces next to the wall are near-parallel to the wall. Clearly, a cylindrical container makes this impossible all the way round. $\endgroup$ – John Bentin Dec 16 '17 at 22:29
  • $\begingroup$ @Carlo : the acceleration being directed downside or perpendicular to the boundary, it just says that the potential energy shall end minimal along both components. $\endgroup$ – jmary Dec 18 '17 at 8:59

This should be seen as a comment, but it is too long for a comment:

One aspect, that has not been addressed in the answers, is the influence of the container geometry. In the experiment, a cylindrical container has been subjected to two different kinds of motions: a coaxial rotation with alternating directions and tapping to the side of side of the cylinder, which can also be interpreted as a horizontal motion that keeps the axis upright.

Assume for a moment, that the experiment were carried out without the influence of gravity and the cubes at least a distance of $\epsilon$ apart. then,

  • Both kinds of motions would result in horizontal motions of the cube's centers of gravity.

  • in the case of rotational motion the primary source of impact on the cubes would be friction between the cylinder and the cubes touching it, resulting in a pure rotation of those cubes around an axis through their center of gravity that is parallel to the one of the container. The "wave of motion" will proceed outside-in as the rotating cubes start to collide and the axes of rotation will start to deviate from the cylinder axis; there will also be forces on the cubes' centers that have a vertical component. All in all, the effects will be fairly moderate.

  • in the case of tapping motion cubes will collide with cylinder and are roughly reflected like rays of light on a mirror, which means that there will be a caustic of the horizontical motion vectors or, put differently, the shockwaves will be bundled and result in a much higher motion energy acting on certain cubes. A secondary effect will be, that after a while cubes will be reflected from the opposite "side" of the cylinder and then collide with other cubes, that are still on their way to that side; the effect will be approximately the same as if two vertically aligned balls are dropped to the ground, namely that the reflection of the second cube will be accelerated towards the cylinder axis again.

So, in a nutshell the difference can be explained by the different magnitude of shockwaves that are generated with the different kinds of motions; that can easily be checked by replacing the cubes with water and measuring the deviation of the surface from equilibrium.

Further experimental investigations could check the effect of container geometry (elliptical or prismatic instead of cylindrical) or rotation aroung an axis off the center of symmetry.
But I am neither a physicist, nor do I have any background in statistical mechanics, so forgive me if my answer is nonsense.

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  • $\begingroup$ Perhaps also the "small-scale" geometry of the interior surfaces, if the bottom surface of the container were irregular at the scale of the cubes (rather than flat), would the emergent pattern differ? $\endgroup$ – J.J. Green Aug 27 at 13:04

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