Argon

The Lennard-Jones model for argon.

Argon (Ar) has a mass of 39.948 umas. Sadus and Prausnitz have shown that three-body repulsion makes a significant contribution to three-body interactions in the liquid phase (for use of the Axilrod-Teller interaction see ). However, the generic Lennard-Jones model has been frequently used due to its simplicity; some parameters are quoted in the next section. A specific interatomic potential for Ar has been proposed by Aziz .

Thermophysical properties (experimental)

Property	Temperature	Pressure
Triple point	83.8058 K	69 kPa
Critical point	150.87 K	4.898 MPa
Melting point	83.80 K
Boiling point	87.30 K

Lennard-Jones parameters

The Lennard-Jones parameters for liquid argon are listed in the following table:

Authors	$\epsilon /k_{B}$ (K)	$\sigma$ (nm)	Reference
Rowley, Nicholson and Parsonage	119.8	0.3405
Barker, Fisher and Watts	142.095	0.33605
White	125.7	0.3345	parameter set #4

Radial distribution function

Radial distribution function

• J. L. Yarnell, M. J. Katz, R. G. Wenzel and S. H. Koenig "Structure Factor and Radial Distribution Function for Liquid Argon at 85°K", Physical Review A 7 pp. 2130-2144 (1973)

Quantum simulations

• J. R. Melrose and K. Singer "An investigation of supercooled Lennard-Jones argon by quantum mechanical and classical Monte Carlo simulation", Molecular Physics 66 1203-1214 (1989)

References

Related material

• H. C. Longuet-Higgins and B. Widom "A rigid sphere model for the melting of argon", Molecular Physics 8 pp. 549-556 (1964)
• D. Henderson and J. A. Barker "On the solidification of argon", Molecular Physics 14 pp. 587-589 (1968)
• F. Lado "Numerical Calculation of the Density Autocorrelation Function for Liquid Argon", Physical Review A 5 pp. 2238-2244 (1972)
• Ali Asghar Davoodi and Farzaneh Feyzi "A new approach for long range corrections in molecular dynamics simulation with application to calculation of argon properties", Journal of Molecular Liquids 150 pp. 33-38 (2009)