2014
DOI: 10.1063/1.4849135
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Nanoparticles at liquid interfaces: Rotational dynamics and angular locking

Abstract: Nanoparticles with different surface morphologies that straddle the interface between two immiscible liquids are studied via molecular dynamics simulations. The methodology employed allows us to compute the interfacial free energy at different angular orientations of the nanoparticle. Due to their atomistic nature, the studied nanoparticles present both microscale and macroscale geometrical features and cannot be accurately modeled as a perfectly smooth body (e.g., spheres, cylinders). Under certain physical c… Show more

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Cited by 22 publications
(48 citation statements)
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“…Alternatively, the contact line can be pinned by kinetic trapping at heterogeneities, roughness or other pinning sites on the particle surface [10,[14][15][16][17][18]. Curvature capillary migration depends on the coupling of the particle-sourced distortion with the host interface shape.…”
Section: Introductionmentioning
confidence: 99%
“…Alternatively, the contact line can be pinned by kinetic trapping at heterogeneities, roughness or other pinning sites on the particle surface [10,[14][15][16][17][18]. Curvature capillary migration depends on the coupling of the particle-sourced distortion with the host interface shape.…”
Section: Introductionmentioning
confidence: 99%
“…A widely used approach to calculate a minimum energy surface is by means of the Surface Evolver program. 42 But several other approaches, both theoretical and numerical, have been used for studying the fluid-fluid interface shape in different physical problems, e.g., menisci shapes and capillary interactions, [43][44][45][46][47][48][49][50][51][52] droplet shapes, [53][54][55][56][57] diffuse interfaces, [58][59][60] or fluid-fluid interfaces in contact with deformable solids. [61][62][63] In this article, we introduce a new numerical method to obtain the minimum-energy shape of a fluid-fluid interface.…”
Section: Introductionmentioning
confidence: 99%
“…Hence, periodic energy barriers ∆U − at regular steps s hinder backward random displacements as the liquid-liquid interface undergoes thermal motion along the terraced surface. The time to cross over an energy barrier induced by nanoscale surface features can be predicted via Kramers theory of thermally-activated transitions, as documented in prior work [9,10]. For the present analysis, it suffices to recognize that a mean time T − ∝ exp(∆U − /k B T ) must elapse before observing a backward displacement of the interface over a terrace edge.…”
mentioning
confidence: 99%
“…At nanoscales, the interplay between intermolecular forces, Brownian motion, and surface structure can give rise to complex interfacial phenomena that challenge conventional, continuum-based and deterministic, models [4][5][6]. For example, nanoscale surface structures can induce wetting processes governed by thermally-activated transitions between multiple metastable states [7][8][9][10][11][12]. These random transitions lead to directed transport of fluids and solutes when there is directional asymmetry of the energy barriers induced by the physicochemical structure of the confining surfaces [13][14][15].…”
mentioning
confidence: 99%
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