Idealised models: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs) m (→'Soft' models:   Slight tidy up.) | Carl McBride (talk | contribs)  m (→'Hard' models) | ||
| Line 26: | Line 26: | ||
| *[[Hard rods]] | *[[Hard rods]] | ||
| *[[hard sphere model | Hard sphere]] | *[[hard sphere model | Hard sphere]] | ||
| **[[Dipolar hard spheres]] | |||
| *[[Hard spherocylinders]] | *[[Hard spherocylinders]] | ||
| *[[Tangent linear hard sphere chains]] | *[[Tangent linear hard sphere chains]] | ||
Revision as of 17:36, 23 January 2008
Lattice models
- Barker-Fock model
- Blume-Emery-Griffiths model (including the Blume-Capel model)
- Bond fluctuation model
- Hard hexagons
- Lattice gas
- Lebwohl-Lasher model
- Potts model
- RP(n-1) model
- N-vector model:
- Ising Models (n=1)
- XY model (n=2)
- Heisenberg model (n=3)
 
'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
- Confined systems
- Flexible molecules (intramolecular interactions)
- Gaussian overlap model
- Gay-Berne model
- Intermolecular Interactions
- Kihara potential
- Lennard-Jones model
- Morse potential
- United-atom model
'Charged' models
Three-body potentials
- Axilrod-Teller interaction
- Silicon
- Many-body interactions - a general discussion page.