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2019
DOI: 10.1103/physreve.100.023101
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Large effect of lateral box size in molecular dynamics simulations of liquid-solid friction

Abstract: Molecular dynamics simulations are a powerful tool to characterize liquid-solid friction. A slab configuration with periodic boundary conditions in the lateral dimensions is commonly used, where the measured friction coefficient could be affected by the finite lateral size of the simulation box. Here we show that for a very wetting liquid close to its melting temperature, strong finite size effects can persist up to large box sizes along the flow direction, typically ∼30 particle diameters. We relate the obser… Show more

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Cited by 15 publications
(10 citation statements)
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References 63 publications
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“…A recent work 59 pointed out that small inhomogeneous systems, under certain conditions, tend to underestimate the solid-liquid friction. However, in this work we have not accounted for this effect, as we focussed solely on the derivation and application of the TTCF formalism under constant pressure conditions for the study of highly confined fluid systems.…”
Section: Methodology and Computation Detailsmentioning
confidence: 99%
“…A recent work 59 pointed out that small inhomogeneous systems, under certain conditions, tend to underestimate the solid-liquid friction. However, in this work we have not accounted for this effect, as we focussed solely on the derivation and application of the TTCF formalism under constant pressure conditions for the study of highly confined fluid systems.…”
Section: Methodology and Computation Detailsmentioning
confidence: 99%
“…The high density of the wall is due to the reduced diameter of the wall particles and corresponds to ρ w = 1 if the quantities were normalized, assuming σ w = 1. A recent work 59 pointed out…”
Section: The Journal Of Chemical Physicsmentioning
confidence: 99%
“…Figure 1 (a) shows the MD simulation system of a quasi-1D Couette-type flow, where the basic setup is a standard one similar to our previous study. 31,32 The two parallel solid walls were fcc crystals and every pair of the nearest neighbors in the walls was bound through a harmonic potential Φ h (r) = k 2 (r − r eq ) 2 , with r being the interparticle distance, r eq = 0.277 nm, and k = 46.8 N/m. Interactions between fluid particles and between fluid and solid particles were modeled by a 12-6 LJ potential…”
Section: A Quasi-1d Couette-type Flowmentioning
confidence: 99%