Strongly correlating liquids: Difference between revisions

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'''Strongly correlating liquids''' are defined as those for whom <math>R \ge 0.9</math> where (Eq. 2 <ref>[http://dx.doi.org/10.1063/1.3582900 Thomas B. Schrøder, Nicoletta Gnan, Ulf R. Pedersen, Nicholas P. Bailey, and Jeppe C. Dyre "Pressure-energy correlations in liquids. V. Isomorphs in generalized Lennard-Jones systems", Journal of Chemical Physics '''134''' 164505 (2011)]</ref>)
'''Strongly correlating liquids''' are defined as those for whom <math>R \ge 0.9</math> where (Eq. 6 <ref>[http://dx.doi.org/10.1063/1.2982247 Nicholas P. Bailey, Ulf R. Pedersen, Nicoletta Gnan, Thomas B. Schrøder, and Jeppe C. Dyre "Pressure-energy correlations in liquids. I. Results from computer simulations", Journal of Chemical Physics '''129''' 184507 (2008)]</ref>)


:<math>R=\frac{\langle \Delta V \Delta U \rangle}{ \sqrt{ \langle (\Delta V)^2 \rangle \langle (\Delta U)^2 \rangle  }  }</math>
:<math>R=\frac{\langle \Delta V \Delta U \rangle}{ \sqrt{ \langle (\Delta V)^2 \rangle \langle (\Delta U)^2 \rangle  }  }</math>
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where <math>\Delta U</math> represents [[Fluctuation theorem | fluctuations]] of the potential  in the [[Canonical ensemble | NVT ensemble]] and <math>V</math>
where <math>\Delta U</math> represents [[Fluctuation theorem | fluctuations]] of the potential  in the [[Canonical ensemble | NVT ensemble]] and <math>V</math>
is the [[virial]] (see also [[Virial pressure]]).
is the [[virial]] (see also [[Virial pressure]]).
==Isomorphs==
<ref>[http://dx.doi.org/10.1063/1.3265957 Nicoletta Gnan, Thomas B. Schrøder, Ulf R. Pedersen, Nicholas P. Bailey, and Jeppe C. Dyre "Pressure-energy correlations in liquids. IV. “Isomorphs” in liquid phase diagrams", Journal of Chemical Physics '''131''' 234504 (2009)]</ref>
==Lennard-Jones liquid==
==Lennard-Jones liquid==
The liquid phase formed by the [[Lennard-Jones model]] is an example of a strongly correlating liquid.
The liquid phase formed by the [[Lennard-Jones model]] is an example of a strongly correlating liquid<ref>[http://dx.doi.org/10.1063/1.3582900 Thomas B. Schrøder, Nicoletta Gnan, Ulf R. Pedersen, Nicholas P. Bailey, and Jeppe C. Dyre "Pressure-energy correlations in liquids. V. Isomorphs in generalized Lennard-Jones systems", Journal of Chemical Physics '''134''' 164505 (2011)]</ref>.
==References==
==References==
<references/>
<references/>
;Related reading
;Related reading
*[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)]
[[category:Complex systems]]
[[category:Complex systems]]

Revision as of 10:43, 18 May 2011

Strongly correlating liquids are defined as those for whom where (Eq. 6 [1])

where represents fluctuations of the potential in the NVT ensemble and is the virial (see also Virial pressure).

Isomorphs

[2]

Lennard-Jones liquid

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

References

Related reading