Lennard-Jones model: Difference between revisions

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* Density: <math> \rho^* := \rho \sigma^3 </math>, where <math> \rho := N/V </math> (number of particles <math> N </math> divided by the volume <math> V </math>)
* Density: <math> \rho^* := \rho \sigma^3 </math>, where <math> \rho := N/V </math> (number of particles <math> N </math> divided by the volume <math> V </math>)
* Temperature: <math> T^* := k_B T/\epsilon </math>, where <math> T </math>  is the absolute [[temperature]] and <math> k_B </math> is the [[Boltzmann constant]]
* Temperature: <math> T^* := k_B T/\epsilon </math>, where <math> T </math>  is the absolute [[temperature]] and <math> k_B </math> is the [[Boltzmann constant]]
The following is a plot of the Lennard-Jones model for the Rowley, Nicholson and Parsonage parameter set <ref>[http://dx.doi.org/10.1016/0021-9991(75)90042-X  L. A. Rowley, D. Nicholson and N. G. Parsonage "Monte Carlo grand canonical ensemble calculation in a gas-liquid transition region for 12-6 Argon", Journal of Computational Physics  '''17''' pp. 401-414 (1975)]</ref> (<math>\epsilon/k_B = </math> 119.8 K and <math>\sigma=</math> 0.3405 nm). See [[argon]] for other parameter sets.
The following is a plot of the Lennard-Jones model for the Rowley, Nicholson and Parsonage parameter set <ref>[http://dx.doi.org/10.1016/0021-9991(75)90042-X  L. A. Rowley, D. Nicholson and N. G. Parsonage "Monte Carlo grand canonical ensemble calculation in a gas-liquid transition region for 12-6 Argon", Journal of Computational Physics  '''17''' pp. 401-414 (1975)]</ref> (<math>\epsilon/k_B = </math> 119.8 K and <math>\sigma=</math> 0.3405 nm). See [[argon]] for other parameter sets.<br>
[[Image:Lennard-Jones.png|500px]]
[[Image:Lennard-Jones.png|500px]]



Revision as of 13:10, 7 April 2010

The Lennard-Jones intermolecular pair potential is a special case of the Mie potential and takes its name from Sir John Edward Lennard-Jones [1] [2] The Lennard-Jones model consists of two 'parts'; a steep repulsive term, and smoother attractive term, representing the London dispersion forces. Apart from being an important model in itself, the Lennard-Jones potential frequently forms one of 'building blocks' of many force fields. It is worth mentioning that the 12-6 Lennard-Jones model is not the most faithful representation of the potential energy surface, but rather its use is widespread due to its computational expediency. One of the first computer simulations using the Lennard-Jones model was undertaken by Rahman in 1964 [3] in a study of liquid argon.

Functional form

The Lennard-Jones potential is given by

Φ12(r)=4ϵ[(σr)12−(σr)6]

where

  • r:=|r1−r2|
  • Φ12(r) is the intermolecular pair potential between two particles or sites
  • σ is the value of r at which Φ12(r)=0
  • ϵ is the well depth (energy)

In reduced units:

  • Density: ρ*:=ρσ3, where ρ:=N/V (number of particles N divided by the volume V)
  • Temperature: T*:=kBT/ϵ, where T is the absolute temperature and kB is the Boltzmann constant

The following is a plot of the Lennard-Jones model for the Rowley, Nicholson and Parsonage parameter set [4] (ϵ/kB= 119.8 K and σ= 0.3405 nm). See argon for other parameter sets.

Special points

  • Φ12(σ)=0
  • Minimum value of Φ12(r) at r=rmin;
rminσ=21/6≃1.12246...

Critical point

The location of the critical point is [5]

Tc*=1.326±0.002

at a reduced density of

ρc*=0.316±0.002.

Vliegenthart and Lekkerkerker [6] have suggested that the critical point is related to the second virial coefficient via the expression

B2|T=Tc=−πσ3

Triple point

The location of the triple point as found by Mastny and de Pablo [7] is

Ttp*=0.694
ρtp*=0.84 (liquid); ρtp*=0.96 (solid)

Approximations in simulation: truncation and shifting

The Lennard-Jones model is often used with a cutoff radius of 2.5σ, beyond which Φ12(r) is set to zero. Setting the well depth ϵ to be 1 in the potential on arrives at Φ12(r)≃−0.0163, i.e. at this distance the potential is at less than 2% of the well depth. See Mastny and de Pablo [7] for an analysis of the effect of this cutoff on the melting line. See Panagiotopoulos for critical parameters [8].

n-m Lennard-Jones potential

It is relatively common to encounter potential functions given by:

Φ12(r)=cn,mϵ[(σr)n−(σr)m].

with n and m being positive integers and n>m. cn,m is chosen such that the minimum value of Φ12(r) being Φmin=−ϵ. Such forms are usually referred to as n-m Lennard-Jones Potential. For example, the 9-3 Lennard-Jones interaction potential is often used to model the interaction between the atoms/molecules of a fluid and a continuous solid wall. On the '9-3 Lennard-Jones potential' page a justification of this use is presented. Another example is the n-6 Lennard-Jones potential, where m is fixed at 6, and n is free to adopt a range of integer values. The potentials form part of the larger class of potentials known as the Mie potential.

See also

Radial distribution function

The following plot is of a typical radial distribution function for the monatomic Lennard-Jones liquid[9] (here with σ=3.73Å and ϵ=0.294 kcal/mol at a temperature of 111.06K):

Typical radial distribution function for the monatomic Lennard-Jones liquid.
Typical radial distribution function for the monatomic Lennard-Jones liquid.

Equation of state

Main article: Lennard-Jones equation of state

Virial coefficients

Main article: Lennard-Jones model: virial coefficients

Phase diagram

Main article: Phase diagram of the Lennard-Jones model

Perturbation theory

The Lennard-Jones model is also used in perturbation theories, for example see: Weeks-Chandler-Anderson perturbation theory.

Mixtures

Related models

References

  1. ↑ John Edward Lennard-Jones "On the Determination of Molecular Fields. I. From the Variation of the Viscosity of a Gas with Temperature", Proceedings of the Royal Society of London. Series A, Containing Papers of a Mathematical and Physical Character 106 pp. 441-462 (1924) § 8 (ii)
  2. ↑ John Edward Lennard-Jones "On the Determination of Molecular Fields. II. From the Equation of State of a Gas", Proceedings of the Royal Society of London. Series A, Containing Papers of a Mathematical and Physical Character 106 pp. 463-477 (1924) Eq. 2.05
  3. ↑ A. Rahman "Correlations in the Motion of Atoms in Liquid Argon", Physical Review 136 pp. A405–A411 (1964)
  4. ↑ L. A. Rowley, D. Nicholson and N. G. Parsonage "Monte Carlo grand canonical ensemble calculation in a gas-liquid transition region for 12-6 Argon", Journal of Computational Physics 17 pp. 401-414 (1975)
  5. ↑ J. M. Caillol " Critical-point of the Lennard-Jones fluid: A finite-size scaling study", Journal of Chemical Physics 109 pp. 4885-4893 (1998)
  6. ↑ G. A. Vliegenthart and H. N. W. Lekkerkerker "Predicting the gas–liquid critical point from the second virial coefficient", Journal of Chemical Physics 112 pp. 5364-5369 (2000)
  7. ↑ 7.0 7.1 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)
  8. ↑ A. Z. Panagiotopoulos "Molecular simulation of phase coexistence: Finite-size effects and determination of critical parameters for two- and three-dimensional Lennard-Jones fluids", International Journal of Thermophysics 15 pp. 1057-1072 (1994)
  9. ↑ John G. Kirkwood, Victor A. Lewinson, and Berni J. Alder "Radial Distribution Functions and the Equation of State of Fluids Composed of Molecules Interacting According to the Lennard-Jones Potential", Journal of Chemical Physics 20 pp. 929- (1952)