Lennard-Jones equation of state

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The equation of state of the Lennard-Jones model.

Contents

[edit] Johnson, Zollweg and Gubbins equation of state

Johnson et al [1] proposed an equation of state based on 33 parameters, which accurately reproduces the vapor liquid equilibrium curve.

[edit] Kolafa and Nezbeda equation of state

The Kolafa and Nezbeda equation of state [2] provides us with the Helmholtz energy function: (Eq. 30):

A = AHS + exp( − γρ2TΔB2,hBH + CijTi / 2ρj
ij

the compressibility factor (Eq. 31)

z \equiv \frac{P}{\rho T}= z_{\mathrm{HS}} +  \rho(1-2\gamma\rho^2) \exp (-\gamma \rho^2) \Delta B_{2,{\mathrm{hBH}}} + \sum_{ij} jC_{ij} T^{i/2-1} \rho^j

and the internal energy (Eq. 32)

U=
 {3(z_{\rm HS}-1)\over d_{\rm hBH}}\,
 {\partial d_{\rm hBH}\over \partial (1/T)}
 + \rho \exp(-\gamma\rho^2)\,{\partial \Delta B_{\rm2,hBH}\over\partial (1/T)}
 - \sum_{ij} \left({i\over2}-1\right) C_{ij}\, T^{i/2} \rho^j

On the following page is the FORTRAN code for the Kolafa and Nezbeda equation of state.

[edit] Melting line

The solid and liquid densities along the melting line are given by the equations of Mastny and de Pablo (Ref [3] Eqs. 20 and 21):

\rho_{\mathrm {solid}} = \beta^{-1/4} \left[ 0.908629 - 0.041510 \beta + 0.514632 \beta^2 -0.708590\beta^3 + 0.428351 \beta^4 -0.095229 \beta^5\right]

and

\rho_{\mathrm {liquid}} = \beta^{-1/4} \left[ 0.90735 - 0.27120 \beta + 0.91784 \beta^2 -1.16270\beta^3 + 0.68012 \beta^4 -0.15284 \beta^5\right]


[edit] References

  1. J. Karl Johnson, John A. Zollweg and Keith E. Gubbins "The Lennard-Jones equation of state revisited", Molecular Physics 78 pp. 591-618 (1993)
  2. Jirí Kolafa, Ivo Nezbeda "The Lennard-Jones fluid: an accurate analytic and theoretically-based equation of state", Fluid Phase Equilibria 100 pp. 1-34 (1994)
  3. Ethan A. Mastny and Juan J. de Pablo "Melting line of the Lennard-Jones system, infinite size, and full potential", Journal of Chemical Physics 127 104504 (2007)

Related reading

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