Idealised models: Difference between revisions

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m (→‎Metals: Added a pair of internal links)
m (Added an internal link to the Harmonic repulsion potential)
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==Piecewise continuous models==
==Piecewise continuous models==
*[[Buldyrev and Stanley model]]
*[[Buldyrev and Stanley model]]
*[[Harmonic repulsion potential]]
*[[Hemmer and Stell model]]
*[[Hemmer and Stell model]]
*[[Hertzian sphere model]]
*[[Hertzian sphere model]]
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**[[Double square well model]]
**[[Double square well model]]
*[[Triangular well model]]
*[[Triangular well model]]
 
*[[Soft sphere potential]]
=='Soft' models==
=='Soft' models==
*[[Born-Huggins-Meyer potential]]
*[[Born-Huggins-Meyer potential]]
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*[[Gaussian overlap model]] (including the Gaussian core model)
*[[Gaussian overlap model]] (including the Gaussian core model)
*[[Gay-Berne model]]
*[[Gay-Berne model]]
*[[Harmonic repulsion potential]]
*[[Intermolecular Interactions]]
*[[Intermolecular Interactions]]
*[[Kihara potential]]
*[[Kihara potential]]
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*[[United-atom model]]
*[[United-atom model]]
*[[Single site anisotropic soft-core potential]]
*[[Single site anisotropic soft-core potential]]
*[[Soft-core square well model]]
*[[Soft sphere potential]]
*[[Soft sphere potential]]



Revision as of 12:12, 26 January 2011

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

'Soft' models

Patchy models

Charged or polar models

Three-body and many-body potentials

Metals