Lubachevsky–Stillinger algorithm: Difference between revisions

Revision as of 05:46, 23 April 2011

Revision as of 06:07, 23 April 2011

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<ref> Packing Hyperspheres in High-Dimensional Euclidean Spaces," M. Skoge, A. Donev, F.H. Stillinger, and S. Torquato, Phys. Rev. E 74, 041127 (2006)</ref>

in using the LSA in dimensions higher than 3.

== Comments on the algorithm ==

ParticleThe state of particle jamming is achieved via simulating

[[granular flow]].

The flow is rendered as a

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with the infinite precision.

Then the jamming would have

occurred [[ad infinitum]],.

after simulating infinitely many

collisions.

In practice, the precision is finite as

is the available resolution of representing

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Volume 34 Issue 2, 1980

</ref>

, the LSA is distinguished by a simpler data structure

and data handling.

For any particle at any stage of calculations