1989
DOI: 10.1080/08927028908031373
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The Force-Biased Algorithm for the Irregular Close Packing of Equal Hard Spheres

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Cited by 85 publications
(79 citation statements)
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“…The particles in [ 12] were not in perfect contact (unlike experimental structures); the average coordination number (defined via surface neighboring within 10 2a) was about 5.4, instead of being slightly above the true value 6. More discouragingly, it was shown in [ 19] for the same order of particle number (N = 1000) that a much slower contraction of the outer diameter results in appreciably higher packing density, up to 0.649-0.650 (see also [23 ] ). Our calculations using the algorithm [ 19] suggests even a higher packing density, at least 0.666 in the limit k~0, N--*~ (see Section 3).…”
Section: Introductionmentioning
confidence: 95%
“…The particles in [ 12] were not in perfect contact (unlike experimental structures); the average coordination number (defined via surface neighboring within 10 2a) was about 5.4, instead of being slightly above the true value 6. More discouragingly, it was shown in [ 19] for the same order of particle number (N = 1000) that a much slower contraction of the outer diameter results in appreciably higher packing density, up to 0.649-0.650 (see also [23 ] ). Our calculations using the algorithm [ 19] suggests even a higher packing density, at least 0.666 in the limit k~0, N--*~ (see Section 3).…”
Section: Introductionmentioning
confidence: 95%
“…Whilst prohibiting crystal nucleation, such a process also misses the 'window' of re-equilibration to access RCP. There is a growing literature [58][59][60] of similar such processes. Some of these 'simulation' phenomena may have no experimental counterpart, and exist only within a computer.…”
Section: Irreversiblementioning
confidence: 99%
“…Such structures resulting from essentially athermal processes have no thermodynamic description. Moreover, they may not meet the same criteria for 'jammed' states, as defined by different compaction processes [58][59][60][61][62]. Beyond around k 1 = 100 the algorithm equations (5)- (8) becomes unstable near close packing when many collision times in equation (8) become less than the smallest precision of the compiler.…”
Section: Irreversiblementioning
confidence: 99%
“…Since the introduction of physical methods for DEM in rock mechanics by Cundall and Strack (1979), also many systems have been developed world-wide in concrete technology; in many cases however this was accomplished for specific and thus restricted purposes. Reference can be given to Jodrey and Torey (1981), Ansell and Dickinson (1986), Mościński et al (1989), Bentz et al (1993), O'Connor et al (1997); Stroeven (1999), Tsunekawa and Iwashita (2001), Puri and Uomoto (2002), Williams and Philipse (2003), Li et al (2006) and Markauskas and Kačia-nauskas (2006). Relevant discussion on this issue can be found in Stroeven et al (2009)…”
Section: Introductionmentioning
confidence: 99%