Content deleted Content added
No edit summary |
No edit summary |
||
Line 31:
combined with a
hard boundary, and the boundary can be mobile.
In a final, compressed, or "jammed" state,
some particles, the so-called "rattlers," are not jammed, they are able to move
within "cages" formed by their immobile, jammed neighbors
and the boundary, if any.
The
target feature
of the LSA, but a real phenomenon,
that the simulation, somewhat unexpectedly, reveals.
Frank Stillinger coined the term from the observation
that if one physically shakes a compressed bunch of hard
particles, some of them, the rattlers, will be rattling.
In the pre-"jammed" mode
Line 46 ⟶ 50:
dynamic [[granular flow]].
Various dynamics of the instantaneous collisions
can be simulated such as: with or without a full restitution,
with or without tangential friction
Differences in masses of the particles can be taken
into account.
Line 54 ⟶ 58:
by decreasing the sizes of all or some of the particles.
Another possible extension of the LSA is replacing
the hard collision [[force]] [[potential]]▼
▲hard collision potential
(zero outside the particle, infinity at or inside) with
a piece
would approximate
a molecular dynamic simulation with continuous
|