Idealised models: Difference between revisions
Jump to navigation
Jump to search
Carl McBride (talk | contribs) |
Carl McBride (talk | contribs) |
||
| Line 53: | Line 53: | ||
==Three-body potentials== | ==Three-body potentials== | ||
*[[Axilrod-Teller interaction]] | |||
*[[Silicon potential | Silicon]] | |||
*[[Many-body interactions]] | *[[Many-body interactions]] | ||
== Metals == | == Metals == | ||
Revision as of 13:54, 6 September 2007
Lattice models
- Hard hexagons
- Heisenberg model
- Ising Models
- XY model
- RP(n-1) model
- Lattice gas
- Lebwohl-Lasher model
- Potts model
- Bond fluctuation model
'Hard' models
- Hard rods
- Hard disks
- Hard sphere
- Widom-Rowlinson model
- Two-dimensional hard dumbbells
- Three-dimensional hard dumbbells
- Tangent linear hard sphere chains
- Flexible hard sphere chains (also known as the pearl-necklace model)
- Branched hard sphere chains
- Fused hard sphere chains
- Hard ellipsoids
- Hard spherocylinders
- Hard core Yukawa
Piecewise continuous models
'Soft' models
- Gaussian overlap model
- Gay-Berne model
- Kihara potential
- Lennard-Jones rods
- Lennard-Jones disks
- Lennard-Jones model
- 9-3 Lennard-Jones potential
- United-atom model
- Intermolecular Interactions
- Flexible molecules (intramolecular interactions)
- Confined systems
'Charged' models
- Restricted primitive model
- Charged hard dumbbells
- Shell model
- Relaxed shell model
- Dynamical shell model (also known as the adiabatic shell model)