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February 28, 2026The Journal of Chemical Physics0 citationsOpen Access

On the importance of numerical integration details for homogeneous flow simulation

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SSStephen K. SandersonDSDebra J. Searles

Key Points

  • The aim is to improve the numerical integration scheme for Sllod equations to ensure energy conservation during simulations.
  • Developed a reversible integration scheme for Sllod equations
  • Implemented the scheme in LAMMPS for simulation
  • Analyzed effects on simulations of transient responses and mixed flows
  • Evaluated error in calculating viscosity at high flow rates.
  • Achieved energy conservation with error on the order of δt3
  • Improved accuracy in simulation of pressure tensor and viscosity
  • Identified significant errors in viscosity at high flow rates without energy conservation.

Abstract

The Sllod equations of motion enable modeling of homogeneous flow at the atomic scale and are commonly used to predict fluid properties such as viscosity. However, few publicly available codes support such simulations, and those that do often include subtle problems in the numerical integration scheme or related aspects, which result in a failure to conserve the energy of the extended system. Here, we demonstrate a reversible and energy-conserving integration scheme for the Sllod equations of motion with error on the order of δt3, in line with typical operator splitting integrators used in standard molecular dynamics simulations. We discuss various implementation details and implement the scheme in LAMMPS, where we find that our changes enable more accurate simulation of transient responses, mixed flows, and steady states, especially at high rates of flow. Importantly, we show that a lack of energy conservation can manifest as a systematic error in the direct ensemble average of the pressure tensor, leading to an error in the calculated viscosity which becomes significant at high flow rates.

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Cite This Study

Sanderson et al. (2026) studied this question.

synapsesocial.com/papers/69a287460a974eb0d3c02e43https://doi.org/10.1063/5.0315430
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