Idealised models: Difference between revisions

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m (→‎'Hard' models: Added an internal link)
(Removed Piecewise continuous links from 'soft' section)
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**[[Soft-core Gay-Berne model]]
**[[Soft-core Gay-Berne model]]
*[[Generalized exponential model]]
*[[Generalized exponential model]]
*[[Harmonic repulsion potential]]
*[[Intermolecular Interactions]]
*[[Intermolecular Interactions]]
*[[Kihara potential]]
*[[Kihara potential]]
Line 114: Line 113:
**[[Lennard-Jones model in 4-dimensions]]  
**[[Lennard-Jones model in 4-dimensions]]  
**[[Lennard-Jones sticks]]
**[[Lennard-Jones sticks]]
**[[modified Lennard-Jones model]]
**[[n-6 Lennard-Jones potential]]
**[[n-6 Lennard-Jones potential]]
**[[8-6 Lennard-Jones potential]]
**[[8-6 Lennard-Jones potential]]
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*[[Single site anisotropic soft-core potential]]
*[[Single site anisotropic soft-core potential]]
*[[Snub hexagonal model]]
*[[Snub hexagonal model]]
*[[Soft-core square well model]]
*[[Soft sphere potential]]
*[[Soft sphere attractive Yukawa model]]
*[[Soft sphere attractive Yukawa model]]
*[[Tietz potential]]
*[[Tietz potential]]

Revision as of 13:44, 13 December 2017

Idealised models usually consist of a simple intermolecular pair potential, whose purpose is often to study underlying physical phenomena, such as generalised phase diagrams and the study of phase transitions. It is entirely possible that a number of the models bear little or no resemblance to real molecular fluids.

Lattice models

'Hard' models

Multi-site models

Piecewise continuous models

Multi-site models

'Soft' models

Multi-site models

Patchy models

Charged or polar models

Three-body and many-body potentials

Metals