Idealised models: Difference between revisions
		
		
		
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m (→'Soft' models)  | 
				Carl McBride (talk | contribs)  m (→Piecewise continuous models:   Added internal link to Hemmer and Stell model)  | 
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==Piecewise continuous models==  | ==Piecewise continuous models==  | ||
*[[Hemmer and Stell model]]  | |||
*[[Ramp model]]  | *[[Ramp model]]  | ||
*[[Square well model]]  | *[[Square well model]]  | ||
Revision as of 12:49, 22 February 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
 - 1-dimensional hard rods
 - 3-dimensional hard rods
 - Hard sphere
 - Hard spherocylinders
 - Sutherland potential
 - Tangent linear hard sphere chains
 - Widom-Rowlinson model
 
Piecewise continuous models
- Hemmer and Stell model
 - Ramp model
 - Square well model
 - Square shoulder model
 - Square shoulder + square well
 - Triangular well model
 
'Soft' models
- Born-Huggins-Meyer potential
 - Buckingham potential
 - Continuous shouldered well model
 - Flexible molecules (intramolecular interactions)
 - Gaussian overlap model
 - Gay-Berne model
 - Intermolecular Interactions
 - Kihara potential
 - Lennard-Jones model
 - Morse potential
 - United-atom model
 - Single site anisotropic soft-core potential
 
Charged or polar models
- Restricted primitive model
 - Charged hard dumbbells
 - Charged hard spherocylinders
 - Shell model
 - Dipolar hard spheres
 - Stockmayer potential
 
Three-body potentials
- Many-body interactions - a general discussion page.
 - Axilrod-Teller interaction