Derivation of a general fluid equation of state based on the quasi-Gaussian entropy theory: application to the Lennard-Jones fluid

In this article we present an equation of state for fluids, based on the quasi-Gaussian entropy theory. The temperature dependence along isochores is described by a confined Gamma state, previously introduced, combined with a simple perturbation term. The 11 parameters occurring in the free energy and pressure expressions along the isochores are obtained from molecular dynamics simulation data. The equation of state has been parametrized for the Lennard-Jones fluid in the (reduced) density range 0–1.0 and (reduced) temperature range 1.0–20.0 using (partly new) NVT molecular dynamics simulation data. An excellent agreement for both energy and pressure was obtained. To test the ability to extrapolate to unknown state points, the parametrization was also performed on a smaller set of data in the temperature range 1.0–6.0. The results in the two cases are remarkably close, even in the high temperature range, and are often almost indistinguishable, in contrast to a pure empirical equation of state, like for ex...

[1]  D. Owen,et al.  Handbook of statistical distributions , 1978 .

[2]  Jean-Pierre Hansen,et al.  Phase Transitions of the Lennard-Jones System , 1969 .

[3]  J. Banavar,et al.  Computer Simulation of Liquids , 1988 .

[4]  A. W. Kemp,et al.  Univariate Discrete Distributions , 1993 .

[5]  M. Kendall,et al.  Kendall's advanced theory of statistics , 1995 .

[6]  J. H. R. Clarke,et al.  A comparison of constant energy, constant temperature and constant pressure ensembles in molecular dynamics simulations of atomic liquids , 1984 .

[7]  I. R. Mcdonald,et al.  Theory of simple liquids , 1998 .

[8]  A. Panagiotopoulos Direct determination of phase coexistence properties of fluids by Monte Carlo simulation in a new ensemble , 1987 .

[9]  G. A. Baker Essentials of Padé approximants , 1975 .

[10]  L. Verlet Computer "Experiments" on Classical Fluids. I. Thermodynamical Properties of Lennard-Jones Molecules , 1967 .

[11]  John S. Rowlinson,et al.  Liquids and liquid mixtures , 1959 .

[12]  David Chandler,et al.  Optimized cluster theory, the Lennard-Jones fluid, and the liquid-gas phase transition , 1974 .

[13]  Andrea Amadei,et al.  Application of the quasi-Gaussian entropy theory to molecular dynamics simulations of Lennard-Jones fluids , 1998 .

[14]  D. Frenkel,et al.  UvA-DARE ( Digital Academic Repository ) Calculation of the chemical potential in the Gibbs ensemble , 2006 .

[15]  W. Kieffer Specialist Periodical Reports , 1975 .

[16]  Ivo Nezbeda,et al.  The Lennard-Jones fluid: an accurate analytic and theoretically-based equation of state , 1994 .

[17]  Athanassios Z. Panagiotopoulos,et al.  Phase equilibria by simulation in the Gibbs ensemble , 1988 .

[18]  H. Berendsen,et al.  Application of the quasi-Gaussian entropy theory to the calculation of thermodynamic properties of water and methane in the liquid and gas phase , 1996 .

[19]  Amyn S. Teja,et al.  AN EQUATION OF STATE FOR REAL FLUIDS BASED ON THE LENNARD-JONES POTENTIAL , 1996 .

[20]  Y. Miyano,et al.  An equation of state for lennard-jones pure fluids applicable over a very wide temperature range , 1993 .

[21]  Jadran Vrabec,et al.  Vapour liquid equilibria of the Lennard-Jones fluid from the NpT plus test particle method , 1992 .

[22]  G. A. Baker,et al.  The Padé approximant in theoretical physics , 1970 .

[23]  J. Barker,et al.  What is "liquid"? Understanding the states of matter , 1976 .

[24]  Denis J. Evans,et al.  Non-Newtonian molecular dynamics , 1984 .

[25]  H. Berendsen,et al.  Extensions of the quasi-Gaussian entropy theory , 1997 .

[26]  A. J. Stam,et al.  Estimation of statistical errors in molecular simulation calculations , 1986 .

[27]  W. Reynolds Thermodynamic properties in SI , 1979 .

[28]  D. J. Tildesley,et al.  Equation of state for the Lennard-Jones fluid , 1979 .

[29]  L. Verlet,et al.  Perturbation Theory and Equation of State for Fluids , 1969 .

[30]  H. Berendsen,et al.  On the use of the quasi-Gaussian entropy theory in noncanonical ensembles. I. Prediction of temperature dependence of thermodynamic properties , 1998 .

[31]  R. Reid,et al.  The Properties of Gases and Liquids , 1977 .

[32]  D. J. Adams,et al.  Calculating the high-temperature vapour line by Monte Carlo , 1976 .

[33]  D. Frenkel,et al.  Computer simulations in the Gibbs ensemble , 1989 .

[34]  John A. Zollweg,et al.  The Lennard-Jones equation of state revisited , 1993 .

[35]  K. E. Starling,et al.  Equation of State for Nonattracting Rigid Spheres , 1969 .

[36]  Roland Span,et al.  An accurate Van der Waals-type equation of state for the Lennard-Jones fluid , 1996 .

[37]  H. Berendsen,et al.  The quasi‐Gaussian entropy theory: Free energy calculations based on the potential energy distribution function , 1996 .

[38]  Gary P. Morriss,et al.  The isothermal/isobaric molecular dynamics ensemble , 1983 .

[39]  B. Smit,et al.  Phase diagrams of Lennard‐Jones fluids , 1992 .