Idealised models: Difference between revisions
Jump to navigation
Jump to search
Carl McBride (talk | contribs) |
Carl McBride (talk | contribs) |
||
| Line 47: | Line 47: | ||
*[[Lennard-Jones rods]] | *[[Lennard-Jones rods]] | ||
*[[Lennard-Jones sticks]] | *[[Lennard-Jones sticks]] | ||
*[[Morse potential]] | |||
*[[United-atom model]] | *[[United-atom model]] | ||
Revision as of 13:13, 22 November 2007
Lattice models
- Barker-Fock model
- Blume-Emery-Griffiths model (including the Blume-Capel model)
- Bond fluctuation model
- Hard hexagons
- Heisenberg model
- Ising Models
- Kac model
- Lattice gas
- Lebwohl-Lasher model
- Potts model
- RP(n-1) model
- XY model
'Hard' models
- Branched hard sphere chains
- Flexible hard sphere chains (also known as the pearl-necklace model)
- Fused hard sphere chains
- Hard core Yukawa
- Hard disks
- Hard dumbbell model
- Hard ellipsoids
- Hard rods
- Hard sphere
- Hard spherocylinders
- Tangent linear hard sphere chains
- Widom-Rowlinson model
Piecewise continuous models
'Soft' models
- 9-3 Lennard-Jones potential
- 10-4-3 Lennard-Jones potential
- Confined systems
- Flexible molecules (intramolecular interactions)
- Gaussian overlap model
- Gay-Berne model
- Intermolecular Interactions
- Kihara potential
- Lennard-Jones disks
- Lennard-Jones model
- Lennard-Jones rods
- Lennard-Jones sticks
- Morse potential
- United-atom model
'Charged' models
- Restricted primitive model
- Charged hard dumbbells
- Shell model
- Relaxed shell model
- Dynamical shell model (also known as the adiabatic shell model)
Three-body potentials
- Axilrod-Teller interaction
- Silicon
- Many-body interactions - a general discussion page.