Newton’s algorithm for discrete classical dynamics

S Søren Toxvaerd (DNRF Centre “Glass and Time,” Department of Science and Environment, Roskilde University , P.O. Box 260, DK-4000 Roskilde,)

Abstract

A recent article in J. Chem. Phys. argues that the two algorithms, the velocity-Verlet and position-Verlet integrators, commonly used in Molecular Dynamics (MD) simulations, are different [L. Ni and Z. Hu, J. Chem. Phys. 161, 226101 (2024)]. However, not only are the two algorithms just different formulations of the same discrete algorithm, but also are other simple discrete algorithms used in MD simulations in the natural sciences. They are all reformulations of the discrete algorithm derived by Newton in 1687 in Proposition I in the very first part of his book Principia. The different reformulations of Newton’s algorithm for discrete dynamics lead to identical discrete dynamics with the same invariances, momentum, angular momentum, and energy as Newton’s analytical dynamics. Hundreds of thousands of MD simulations with Newton’s discrete dynamics have appeared but unfortunately with many recorded errors for energies, potential energies, temperatures, and heat capacities. The public software for MD should be corrected.

Article Details

Volume / Issue Vol. 162, Issue 2
Published January 14, 2025
ISSN 0021-9606
Publisher American Institute of Physics

Journal Info

The Journal of Chemical Physics

American Institute of Physics

ISSN: 0021-9606 Physical Sciences

Authors (1)

S

Søren Toxvaerd

DNRF Centre “Glass and Time,” Department of Science and Environment, Roskilde University , P.O. Box 260, DK-4000 Roskilde,