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]] simulation | It was generated by the appropriate fitting of very precise [[molecular dynamics]] simulation | ||
results | results | ||
<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" | <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" Physical Chemistry Chemical Physics '''6''' pp. 2335- (2004)] </ref>. This equation is much more precise than [[Carnahan-Starling equation of state|Carnahan-Starling]] equation of state. | ||
== References == | == References == | ||
<references /> | <references /> | ||
[[category: Equations of state]] | [[category: Equations of state]] | ||
Revision as of 12:10, 9 March 2009
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The Kolafa-Labík-Malijevský equation of state 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 [1]. This equation is much more precise than Carnahan-Starling equation of state.