Structural behavior of supercritical fluids under confinement
Kanka Ghosh, C.V.Krishnamurthy

TL;DR
This study investigates how supercritical Lennard-Jones fluids behave structurally under partial confinement, revealing layering and ordering effects that vary with wall rigidity and regime, impacting the structure-dynamics relationship.
Contribution
It provides new insights into the structural changes of supercritical fluids under confinement across the Frenkel line, highlighting the effects of wall rigidity and confinement type.
Findings
Layering and increased order with wall rigidity
Distinct layering patterns for atomistic and reflective walls
Heterogeneity affects structure-dynamics scaling
Abstract
The location of the Frenkel line (FL) of a Lennard-Jones fluid which demarcates two distinct physical states, liquidlike and gaslike within the supercritical regime, has been established through molecular dynamics (MD) simulations of the velocity auto-correlation (VACF) and Radial distribution Function (RDF). We, in this article, explore the changes in the structural features of supercritical LJ-fluid under partial confinement using atomistic walls. The study is carried out across the FL through a series of MD simulations considering a set of thermodynamics states in the supercritical regime of Argon well above the critical point. Confinement is partial, with atomistic walls located normal to z and extending to "infinity" along the x and y directions. In the "liquidlike" regime of the supercritical phase, particles are distributed in distinct layers along the z with layer spacing less…
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