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Line 41: simulating dynamic [[granular flow]]. Various dynamics of the instantaneous collisions can be simulated: with or without a full restitution, with or without tangential friction, and so on. Differences in particles' masses can be taken into account. It is also easy and sometimes proves useful to un-"jam" or "fluidize" the configuration, Line 152 ⟶ 156: to its completeness on the approach to such a time. The ~~same~~ "stuck in time" failure can also occur when using the LSA just for simulating a granular flow,

Lubachevsky–Stillinger algorithm: Difference between revisions