Abstract

Resolving atomic scale details while capturing long-range elastic deformation is the principal difficulty when solving contact mechanics problems with computer simulations. Fully atomistic simulations must consider large blocks of atoms to support long-wavelength deformation modes, meaning that most atoms are far removed from the region of interest. Building on earlier methods that used elastic surface Green's functions to compute static substrate deformation, we present a numerically efficient dynamic Green's function technique to treat realistic, time-evolving, elastic solids. Our method solves substrate dynamics in reciprocal space and utilizes precomputed Green's functions that exactly reproduce elastic interactions without retaining the atomic degrees of freedom in the bulk. We invoke physical insights to determine the necessary number of explicit substrate layers required to capture the attenuation of subsurface waves as a function of surface wave vector. We observe that truncating substrate dynamics at depths that fall as a power of wave vector allows us to accurately model wave propagation without implementing arbitrary damping. The framework we have developed substantially accelerates molecular dynamics simulations of large elastic substrates. We apply the method to single asperity contact, impact, and sliding friction problems and present our preliminary findings.

Highlights

  • Mechanical contacts occur in many technical and biological systems, and they determine our experience with our surroundings through touch or when walking

  • We observe that truncating substrate dynamics at depths that fall as a power of wave vector allows us to accurately model wave propagation without implementing arbitrary damping

  • Molecular dynamics (MD) simulations are a powerful tool commonly used for studying mechanics at

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Summary

INTRODUCTION

Mechanical contacts occur in many technical and biological systems, and they determine our experience with our surroundings through touch or when walking. Bulk DOF can be integrated out for full molecular models of crystalline substrates, leading to lattice surface Green’s functions [23,24] Those formulations have proven successful in quickly and efficiently determining the elastic deformation induced by quasistatically applied interfacial forces. We note that analytic dynamic Green’s functions for semiinfinite substrates have been derived by Kajita et al [28,29,30], who presented an elegant solution to the time-dependent contact problem without adding explicit damping [29,30] Their technique differs from ours in that they use a memory kernel to capture subsurface DOF (see [14,15,16,17] for the equivalent continuum formulation). Since we operate in real space, implementation is simple and compatible with existing massively parallel MD software packages, e.g., LAMMPS [38], which we used for the simulations described in this paper

DAMPING OF EXCITED MODES
THE DYNAMIC CONTACT GREEN’S FUNCTION METHOD
Explicit atoms
Harmonic approximation
Reduction of the dynamic degrees of freedom
Kelvin damping
Parallel scaling and time complexity
EFFECT OF DAMPING PARAMETER ON WAVE
COMPARISON WITH ATOMIC SIMULATIONS
DEMONSTRATION OF ERROR
APPLICATION TO SLIDING FRICTION
VIII. CONCLUSIONS
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