Lennard-Jones fluid#

Simulations of the Lennard-Jones fluid: Rahman’s liquid argon, the Maxwell-Boltzmann speed distribution, hard-sphere-like packing order, the Weeks-Chandler-Andersen repulsive reference fluid, Verlet’s integrator and neighbor list, and self-diffusion from the Einstein mean-squared displacement and the Green-Kubo velocity autocorrelation.

Rahman’s liquid argon: g(r) of a Lennard-Jones liquid in real units

Rahman's liquid argon: g(r) of a Lennard-Jones liquid in real units

Cross-checking an MD trajectory against the Maxwell-Boltzmann distribution

Cross-checking an MD trajectory against the Maxwell-Boltzmann distribution

Alder and Wainwright’s hard spheres: packing-driven order with no attraction

Alder and Wainwright's hard spheres: packing-driven order with no attraction

Weeks-Chandler-Andersen: repulsive forces set the structure of a dense liquid

Weeks-Chandler-Andersen: repulsive forces set the structure of a dense liquid

Verlet’s integrator: bounded energy error instead of drift

Verlet's integrator: bounded energy error instead of drift

Verlet’s neighbor list: a skin that lets one pair list serve many steps

Verlet's neighbor list: a skin that lets one pair list serve many steps

Einstein’s diffusion law: mean-squared displacement grows linearly in time

Einstein's diffusion law: mean-squared displacement grows linearly in time

Green-Kubo: the diffusion coefficient as the integral of the velocity autocorrelation

Green-Kubo: the diffusion coefficient as the integral of the velocity autocorrelation