Math 2.0

Statistical mechanics, structure of matter Classical fluids and liquids Example

Lennard-Jones potential

Builds on Mayer f-functionHard spheres

Example

Let r>0r > 0 be the distance between two neutral atoms. The Lennard-Jones potential is the pair potential V(r)=4ε[(σr)12−(σr)6],V(r) = 4 \varepsilon \left[ \left( \frac{\sigma}{r} \right)^{12} - \left( \frac{\sigma}{r} \right)^{6} \right], where ε>0\varepsilon > 0 is the depth of the well and σ>0\sigma > 0 is the distance at which VV vanishes. The r−12r^{-12} term models short-range repulsion, and the r−6r^{-6} term the van der Waals attraction.

Check of the shape: V(σ)=4ε(1−1)=0V(\sigma) = 4\varepsilon (1 - 1) = 0. The derivative is V′(r)=4ε(−12σ12r−13+6σ6r−7)V'(r) = 4\varepsilon \left( -12 \sigma^{12} r^{-13} + 6 \sigma^6 r^{-7} \right), which vanishes when r6=2σ6r^6 = 2 \sigma^6, that is at rm=21/6σr_m = 2^{1/6} \sigma. There (σ/rm)6=1/2(\sigma/r_m)^6 = 1/2, so V(rm)=4ε(14−12)=−εV(r_m) = 4\varepsilon (\frac14 - \frac12) = -\varepsilon, the minimum. As r→0r \to 0, V(r)→+∞V(r) \to +\infty, and as r→∞r \to \infty, V(r)→0V(r) \to 0 from below.

Remarks

A classical fluid of particles with this pair potential is the standard test system for simulations by molecular dynamics and Monte Carlo methods. Its Mayer f-function f(r)=e−βV(r)−1f(r) = e^{-\beta V(r)} - 1 is close to −1-1 for rr well below σ\sigma, and positive near the well, so the second virial coefficient changes sign with temperature. Unlike hard spheres, the Lennard-Jones fluid has an attractive part and so shows a liquid–gas transition with a critical point.

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  1. Canonical ensemble concept
  2. Mayer f-function concept
  3. Hard spheres example
  4. Lennard-Jones potential example

Further reading

  1. Web https://en.wikipedia.org/wiki/Lennard-Jones_potential
About this page
Tag349MN3ER54
URIm2://349MN3ER54
Kindexample
WritingW0 stub
MSC82B21, 82D15
IllustratesMayer f-function
UsesMayer f-function, Hard spheres
Same as
Changed3 November 2026

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