Idealised models: Difference between revisions
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=='Hard' models== | =='Hard' models== | ||
*[[ | *[[Branched hard sphere chains]] | ||
*[[Flexible hard sphere chains]] (also known as the ''pearl-necklace model'') | *[[Flexible hard sphere chains]] (also known as the ''pearl-necklace model'') | ||
*[[Fused hard sphere chains]] | *[[Fused hard sphere chains]] | ||
*[[Hard core Yukawa]] | |||
*[[Hard disks]] | |||
*[[Hard ellipsoids]] | *[[Hard ellipsoids]] | ||
*[[Hard rods]] | |||
*[[hard sphere model | Hard sphere]] | |||
*[[Hard spherocylinders]] | *[[Hard spherocylinders]] | ||
*[[ | *[[Tangent linear hard sphere chains]] | ||
*[[Three-dimensional hard dumbbells]] | |||
*[[Two-dimensional hard dumbbells]] | |||
*[[Widom-Rowlinson model]] | |||
==Piecewise continuous models== | ==Piecewise continuous models== | ||
Revision as of 15:47, 25 September 2007
Lattice models
- 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 ellipsoids
- Hard rods
- Hard sphere
- Hard spherocylinders
- Tangent linear hard sphere chains
- Three-dimensional hard dumbbells
- Two-dimensional hard dumbbells
- Widom-Rowlinson model
Piecewise continuous models
'Soft' models
- Gaussian overlap model
- Gay-Berne model
- Kihara potential
- Lennard-Jones rods
- Lennard-Jones disks
- Lennard-Jones model
- Lennard-Jones sticks
- 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)
Three-body potentials
- Axilrod-Teller interaction
- Silicon
- Many-body interactions - a general discussion page.