2017
DOI: 10.1039/c6sm02065h
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Maximally dense random packings of cubes and cuboids via a novel inverse packing method

Abstract: The packings of cubes and cuboids (i.e., "elongated" or "compressed" cubes) are ubiquitous in nature. The high symmetry and space-tiling nature of such particles make them easily packable in dense configurations with a high degree of orientational and translational order. In this paper, we devise a novel inverse packing method that enables one to generate dense hard-particle packings with a controllable degree of disorder/order quantified by predefined order metrics via stochastic Monte Carlo optimizations. We… Show more

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Cited by 34 publications
(26 citation statements)
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References 53 publications
(75 reference statements)
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“…For f larger than B0.6, we observe akin to ref. [39][40][41][42] that ordering and orientational correlations start manifesting themselves (for f Z 0.57, crystallization behaviour has been observed). It can hence be discussed whether these configurations are random and to what extent; herein, it suffices to conclude that our algorithm will create crystals for high solid volume fractions.…”
Section: Resultsmentioning
confidence: 94%
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“…For f larger than B0.6, we observe akin to ref. [39][40][41][42] that ordering and orientational correlations start manifesting themselves (for f Z 0.57, crystallization behaviour has been observed). It can hence be discussed whether these configurations are random and to what extent; herein, it suffices to conclude that our algorithm will create crystals for high solid volume fractions.…”
Section: Resultsmentioning
confidence: 94%
“…Just to give a brief account, studies performed include the random close packing of ellipsoids, 27 monodisperse and polydisperse hard spheres, 28,29 polyhedra including platonic solids, [30][31][32][33] superballs and superellipsoids, [34][35][36] cubes with round edges, 37 and monodisperse and polydisperse cubes and cuboids. [38][39][40][41][42] Hard cubes and cuboids and their packing and phase behavior have been studied both as limiting cases of superballs and superellipsoids, 35,36 and modeled exactly as cubes and cuboids. [39][40][41] The true nature of their behavior is somewhat elusive; as stated by Jiao and Torquato, 31 attempts to create random close packings (or rather maximally random jammed packings) of cubes easily lead to high degrees of order, raising questions concerning the appropriateness of some of the algorithms suggested so far to generate these packings.…”
Section: Introductionmentioning
confidence: 99%
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“…41 The MDRP is defined as the densest packing in the random state in which the particle positions and orientations are randomly distributed. [31][32][33]42 The packing density of the MDRP corresponds to a sharp transition in the order map, which characterizes the onset of nontrivial spatial correlations among the particles. 33,42 The MDRP is also regarded as a glass state of hard particle systems with an artificial constraint and is always random.…”
Section: Introductionmentioning
confidence: 99%
“…33,42 The MDRP is also regarded as a glass state of hard particle systems with an artificial constraint and is always random. 31 The jammed or mechanically stable condition is emphasized in the MRJ state, while the random condition is emphasized in the MDRP state. For the particle shapes which are difficult to crystalize, the packing density of the MDRP is close to that of the RCP or MRJ packing, such as the spheroids, 32 spherocylinders, 33 octahedra, 42 and superellipsoids with small surface shape parameters.…”
Section: Introductionmentioning
confidence: 99%