Editing Argon
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'''Argon''' (Ar) has long been a popular choice for [[Computer simulation techniques |computer simulations]] of simple liquids. Some of the first computer simulations of liquid argon were those of Wood and Parker in 1957 <ref>[http://dx.doi.org/10.1063/1.1743822 W. W. Wood and F. R. Parker "Monte Carlo Equation of State of Molecules Interacting with the Lennard‐Jones Potential. I. A Supercritical Isotherm at about Twice the Critical Temperature", Journal of Chemical Physics '''27''' pp. 720- (1957)]</ref> and of Rahman in 1964 <ref name="Rahman">[http://dx.doi.org/10.1103/PhysRev.136.A405 A. Rahman "Correlations in the Motion of Atoms in Liquid Argon", Physical Review '''136''' pp. A405–A411 (1964)]</ref>. Sadus and Prausnitz have shown that three-body repulsion makes a significant contribution to [[Idealised models#Three-body potentials|three-body interactions]] in the liquid phase | '''Argon''' (Ar) has long been a popular choice for [[Computer simulation techniques |computer simulations]] of simple liquids. Some of the first computer simulations of liquid argon were those of Wood and Parker in 1957 <ref>[http://dx.doi.org/10.1063/1.1743822 W. W. Wood and F. R. Parker "Monte Carlo Equation of State of Molecules Interacting with the Lennard‐Jones Potential. I. A Supercritical Isotherm at about Twice the Critical Temperature", Journal of Chemical Physics '''27''' pp. 720- (1957)]</ref> and of Rahman in 1964 <ref name="Rahman" >[http://dx.doi.org/10.1103/PhysRev.136.A405 A. Rahman "Correlations in the Motion of Atoms in Liquid Argon", Physical Review '''136''' pp. A405–A411 (1964)]</ref>. Sadus and Prausnitz have shown that three-body repulsion makes a significant contribution to [[Idealised models#Three-body potentials|three-body interactions]] in the liquid phase | ||
<ref>[http://dx.doi.org/10.1063/1.471172 Richard J. Sadus and J. M. Prausnitz "Three-body interactions in fluids from molecular simulation: Vapor–liquid phase coexistence of argon", Journal of Chemical Physics '''104''' pp. 4784-4787 (1996)]</ref> | <ref>[http://dx.doi.org/10.1063/1.471172 Richard J. Sadus and J. M. Prausnitz "Three-body interactions in fluids from molecular simulation: Vapor–liquid phase coexistence of argon", Journal of Chemical Physics '''104''' pp. 4784-4787 (1996)]</ref> | ||
(for use of the [[Axilrod-Teller interaction]] see | (for use of the [[Axilrod-Teller interaction]] see | ||
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| Authors || <math>\epsilon/k_B</math> (K) || <math>\sigma</math> (nm)|| Reference (year) | | Authors || <math>\epsilon/k_B</math> (K) || <math>\sigma</math> (nm)|| Reference (year) | ||
|- | |- | ||
| Rahman || 120 || 0.34 || <ref name="Rahman"></ref> (1964) | | Rahman || 120 || 0.34 || <ref name="Rahman"> </ref> (1964) | ||
|- | |- | ||
|Barker, Fisher and Watts ||142.095 || 0.33605 || <ref>[http://dx.doi.org/10.1080/00268977100101821 J. A. Barker, R. A. Fisher and R. O. Watts "Liquid argon: Monte carlo and molecular dynamics calculations", Molecular Physics '''21''' pp. 657-673 (1971)]</ref> (1971) | |Barker, Fisher and Watts ||142.095 || 0.33605 || <ref>[http://dx.doi.org/10.1080/00268977100101821 J. A. Barker, R. A. Fisher and R. O. Watts "Liquid argon: Monte carlo and molecular dynamics calculations", Molecular Physics '''21''' pp. 657-673 (1971)]</ref> (1971) | ||
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==Surface tension== | ==Surface tension== | ||
[[Surface tension]] <ref>[http://dx.doi.org/10.1063/1.4885351 Florent Goujon, Patrice Malfreyt and Dominic J. Tildesley "The gas-liquid surface tension of argon: A reconciliation between experiment and simulation", Journal of Chemical Physics '''140''' 244710 (2014)]</ref>. | [[Surface tension]] <ref>[http://dx.doi.org/10.1063/1.4885351 Florent Goujon, Patrice Malfreyt and Dominic J. Tildesley "The gas-liquid surface tension of argon: A reconciliation between experiment and simulation", Journal of Chemical Physics '''140''' 244710 (2014)]</ref>. | ||
==References== | ==References== | ||
<references/> | <references/> |