Lennard-Jones model

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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 its-self, the Lennard-Jones potential frequently forms one of 'building blocks' of may force fields,

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 diameter (length), i.e. 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 parameters ϵ/kB≈ 120 K and σ≈ 0.34 nm. See argon for different parameter sets.

This figure was produced using gnuplot with the command:

plot (4*120*((0.34/x)**12-(0.34/x)**6))

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 [3]

Tc*=1.326±0.002

at a reduced density of

ρc*=0.316±0.002.

Vliegenthart and Lekkerkerker [4] 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 (Ref. 4) 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. See Mastny and de Pablo [5] for an analysis of the effect of this cutoff on the melting line.

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.

Radial distribution function

The following plot is of a typical radial distribution function for the monatomic Lennard-Jones liquid[6] (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