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Lennard-Jones Potential

1924
  • John Lennard-Jones
Laboratory scene with scientist performing molecular dynamics simulations using Lennard-Jones potential.

(generated image for illustration only)

A simple, widely used mathematical model that approximates the potential energy of interaction between two neutral atoms or molecules. It combines a long-range attractive term (\(\propto r^{-6}\)) representing Van der Waals forces with a steep, short-range repulsive term (\(\propto r^{-12}\)) representing Pauli repulsion. The formula is \(V_{LJ}(r) = 4\epsilon [(\frac{\sigma}{r})^{12} – (\frac{\sigma}{r})^6]\).

The Lennard-Jones potential is a cornerstone of computational physics and chemistry due to its simplicity and effectiveness in capturing the essential physics of atomic interactions. The potential describes two main features. The attractive part, \(-(\frac{\sigma}{r})^6\), models the London dispersion force, which dominates at medium to long ranges. The \(r^{-6}\) dependence is theoretically justified for the interaction between two induced dipoles. The repulsive part, \(+(\frac{\sigma}{r})^{12}\), models the strong repulsion that occurs when two atoms get very close and their electron clouds begin to overlap. This repulsion is a consequence of the Pauli exclusion principle. The \(r^{-12}\) form was chosen primarily for computational convenience (as the square of the \(r^{-6}\) term), though it provides a reasonable approximation of the steep repulsive wall.

The two parameters in the model have clear physical meanings: \(\epsilon\) (epsilon) is the depth of the potential well, representing the strength of the attraction, and \(\sigma\) (sigma) is the distance at which the potential energy is zero, representing the effective diameter of the atom. Despite being an approximation, the Lennard-Jones potential is remarkably successful at predicting the properties of simple, nonpolar substances and serves as a fundamental building block for more complex force fields used to simulate proteins, polymers, and other materials.

UNESCO Nomenclature: 2202
– Atomic and molecular physics

Type

Mathematical Model

Disruption

Foundational

Usage

Widespread Use

Precursors

  • Theories of Van der Waals forces (Keesom, Debye, London)
  • The Pauli Exclusion Principle from quantum mechanics
  • The Mie potential, a more general form of interatomic potential
  • Early work on equations of state for real gases

Applications

  • molecular dynamics (MD) and Monte Carlo (MC) simulations of simple fluids, solids, and gases
  • computational chemistry and materials science for developing force fields
  • modeling thermodynamic properties and phase diagrams of substances like argon
  • providing a basic model for interatomic forces in physics education

Patents:

NA

Potential Innovations Ideas

  • development of highly optimized force fields for protein folding simulations and drug discovery
  • ai-based methods to derive accurate interatomic potentials directly from quantum mechanical data
  • real-time simulation of material fracture and stress propagation
  • virtual screening of materials for gas storage (e.g., hydrogen, CO2) applications
  • design of self-assembling nanostructures through computer simulation
  • predictive modeling of viscosity and transport properties in novel liquid mixtures
  • simulators for studying the early stages of crystal nucleation and growth
  • educational software for interactive exploration of atomic forces and phase transitions
  • algorithms for designing materials with negative thermal expansion
  • creation of digital twins for chemical reactors to optimize performance
Related to: Lennard-Jones potential, molecular dynamics, potential energy, intermolecular force, Pauli repulsion, Van der Waals, computational chemistry, simulation, force field, argon.

Historical Context

Lennard-Jones Potential

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1927

(if date is unknown or not relevant, e.g. "fluid mechanics", a rounded estimation of its notable emergence is provided)

10th year anniversary

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