Lennard-Jones model: Difference between revisions
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* <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math> | * <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math> | ||
* <math> \Phi_{12}(r) </math> is the [[intermolecular pair potential]] between two particles or ''sites'' | * <math> \Phi_{12}(r) </math> is the [[intermolecular pair potential]] between two particles or ''sites'' | ||
* <math> \sigma </math> is | * <math> \sigma </math> is the value of <math>r</math> at which <math> \Phi_{12}(r)=0</math> | ||
* <math> \epsilon </math> is the well depth (energy) | * <math> \epsilon </math> is the well depth (energy) | ||
In reduced units: | In reduced units: |
Revision as of 14:39, 6 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
where
- is the intermolecular pair potential between two particles or sites
- is the value of at which
- is the well depth (energy)
In reduced units:
- Density: , where (number of particles divided by the volume )
- Temperature: , where is the absolute temperature and is the Boltzmann constant
The following is a plot of the Lennard-Jones model for the parameters 120 K and 0.34 nm. See argon for different parameter sets.

Special points
- Minimum value of at ;
Critical point
The location of the critical point is [4]
at a reduced density of
- .
Vliegenthart and Lekkerkerker [5] have suggested that the critical point is related to the second virial coefficient via the expression
Triple point
The location of the triple point as found by Mastny and de Pablo [6] is
- (liquid); (solid)
Approximations in simulation: truncation and shifting
The Lennard-Jones model is often used with a cutoff radius of , beyond which is set to zero. Setting the well depth to be 1 in the potential on arrives at , i.e. at this distance the potential is at less than 2% of the well depth. See Mastny and de Pablo [6] for an analysis of the effect of this cutoff on the melting line. See Panagiotopoulos for critical parameters [7].
n-m Lennard-Jones potential
It is relatively common to encounter potential functions given by:
with and being positive integers and . is chosen such that the minimum value of being . 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 is fixed at 6, and 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
- 8-6 Lennard-Jones potential
- 9-3 Lennard-Jones potential
- 9-6 Lennard-Jones potential
- 10-4-3 Lennard-Jones potential
- n-6 Lennard-Jones potential
Radial distribution function
The following plot is of a typical radial distribution function for the monatomic Lennard-Jones liquid[8] (here with and kcal/mol at a temperature of 111.06K):

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
- Kihara potential
- Lennard-Jones model in 1-dimension (rods)
- Lennard-Jones model in 2-dimensions (disks)
- Lennard-Jones model in 4-dimensions
- Lennard-Jones sticks
- Mie potential
- Soft-core Lennard-Jones model
- Soft sphere potential
- Stockmayer potential
References
- ↑ 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)
- ↑ 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
- ↑ A. Rahman "Correlations in the Motion of Atoms in Liquid Argon", Physical Review 136 pp. A405–A411 (1964)
- ↑ J. M. Caillol " Critical-point of the Lennard-Jones fluid: A finite-size scaling study", Journal of Chemical Physics 109 pp. 4885-4893 (1998)
- ↑ 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)
- ↑ Jump up to: 6.0 6.1 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)
- ↑ 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)
- ↑ 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)