Abstract:We identify putatively maximally dense packings of tangent-sphere trimers with fixed bond angles (θ = θ0) using a novel method, and contrast them to the disordered jammed states they form under quasistatic and dynamic athermal compression. Incommensurability of θ0 with 3D closepacking does not by itself inhibit formation of dense 3D crystals; all θ0 allow formation of crystals with φmax(θ0) > 0.97φcp. Trimers are always able to arrange into periodic structures composed of close-packed bilayers or trilayers of … Show more
“…Remarkably, a consistent trend was also found in the jammed packing of this species in 3D. 78 As for ITD and COD, the relative radius g r 1 and maximal overlap magnitude g o 1 determine their shapes (or configurations), yielding saturated packing densities, respectively. Specifically, COD just degenerates into a dimer with a single parameter.…”
Particle morphology is one of the most significant factors influencing packing structures of granular materials. With certain targeted properties or optimization criteria, inverse packing problems have drawn extensive attention in...
“…Remarkably, a consistent trend was also found in the jammed packing of this species in 3D. 78 As for ITD and COD, the relative radius g r 1 and maximal overlap magnitude g o 1 determine their shapes (or configurations), yielding saturated packing densities, respectively. Specifically, COD just degenerates into a dimer with a single parameter.…”
Particle morphology is one of the most significant factors influencing packing structures of granular materials. With certain targeted properties or optimization criteria, inverse packing problems have drawn extensive attention in...
A neural-network-biased genetic algorithm is employed to design model glass formers exhibiting extremes of fragility of glass formation, elucidating connections between molecular geometry, thermodynamics, fragility, and glass-transition temperature.
Many polymers and fibers lie between the flexible limit where “molecules” are random-walk-like and the stiff limit where they are rodlike. We study how these systems' athermal solidification varies throughout the intermediate, semiflexible regime.
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