Strongly correlating liquids: Difference between revisions

Latest revision as of 17:18, 16 February 2012

Strongly correlating liquids are defined as those for whom $R\geq 0.9$ where (Eq. 6 ^[1])

R={\frac {\langle \Delta {\mathcal {V}}\Delta U\rangle }{\sqrt {\langle (\Delta {\mathcal {V}})^{2}\rangle \langle (\Delta U)^{2}\rangle }}}

where $\Delta U$ represents fluctuations of the potential in the NVT ensemble and ${\mathcal {V}}$ is the virial (see also Virial pressure).

The liquid phase formed by the Lennard-Jones model is an example of a strongly correlating liquid^[3].

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 *[http://dx.doi.org/10.1063/1.2982249 Nicholas P. Bailey, Ulf R. Pedersen, Nicoletta Gnan, Thomas B. Schrøder, and Jeppe C. Dyre "Pressure-energy correlations in liquids. II. Analysis and consequences", Journal of Chemical Physics '''129''' 184508 (2008)]
 *[http://dx.doi.org/10.1063/1.3265955 Thomas B. Schrøder, Nicholas P. Bailey, Ulf R. Pedersen, Nicoletta Gnan, and Jeppe C. Dyre "Pressure-energy correlations in liquids. III. Statistical mechanics and thermodynamics of liquids with hidden scale invariance", Journal of Chemical Physics '''131''' 234503 (2009)]
+*[http://dx.doi.org/10.1063/1.3685804  Trond S. Ingebrigtsen, Lasse Bøhling, Thomas B. Schrøder, and Jeppe C. Dyre "Communication: Thermodynamics of condensed matter with strong pressure-energy correlations", Journal of Chemical Physics '''136''' 061102 (2012)]
 [[category: Classical thermodynamics]]
 [[category: Statistical mechanics]]