Kolafa-Labík-Malijevský equation of state: Difference between revisions
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It was generated by the appropriate fitting of very precise [[Molecular dynamics|Molecular dynamics]] simulation | It was generated by the appropriate fitting of very precise [[Molecular dynamics|Molecular dynamics]] simulation | ||
results. See Ref <Ref | results. See Ref <Ref | ||
<ref> [http://dx.doi.org/10.1039/b402792b Jirí Kolafa, Stanislav Labík and Anatol Malijevský, "Accurate equation of state of the hard sphere fluid in stable and metastable regions" Phys. Chem. Chem. Phys. '''6''', 2335 (2004)] </ref> | <ref> [http://dx.doi.org/10.1039/b402792b Jirí Kolafa, Stanislav Labík and Anatol Malijevský, "Accurate equation of state of the hard sphere fluid in stable and metastable regions" Phys. Chem. Chem. Phys. '''6''', 2335 (2004)] </ref>. This equation is much more precise that [[Carnahan-Starling equation of state|Carnahan-Starling]] Equation of State. | ||
== References == | == References == | ||
<references /> | <references /> | ||
Revision as of 18:24, 5 March 2009
This is an equation of state for the fluid phase of three-dimensional hard spheres. It was generated by the appropriate fitting of very precise Molecular dynamics simulation results. See Ref [1]. This equation is much more precise that Carnahan-Starling Equation of State.