Search results for "Wetting transition"

showing 4 items of 34 documents

Toward a density functional description of liquid pH2.

2010

A finite-temperature density functional approach to describe the properties of parahydrogen in the liquid-vapor coexistence region is presented. The first proposed functional is zero-range, where the density-gradient term is adjusted so as to reproduce the surface tension of the liquid-vapor interface at low temperature. The second functional is finite-range and, while it is fitted to reproduce bulk pH2 properties only, it is shown to yield surface properties in good agreement with experiments. These functionals are used to study the surface thickness of the liquid-vapor interface, the wetting transition of parahydrogen on a planar Rb model surface, and homogeneous cavitation in bulk liquid…

Surface (mathematics)Chemical Physics (physics.chem-ph)Statistical Mechanics (cond-mat.stat-mech)Yield surfaceChemistryThermodynamicsFOS: Physical sciencesFísicaCondensed Matter - Soft Condensed MatterSpin isomers of hydrogenFunctional descriptionSurface tensionPhysics::Fluid DynamicsPlanarWetting transitionPhysics - Chemical PhysicsCavitationPhysics::Atomic and Molecular ClustersSoft Condensed Matter (cond-mat.soft)Physical and Theoretical ChemistryCondensed Matter - Statistical MechanicsThe journal of physical chemistry. A
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Droplets pinned at chemically inhomogenous substrates: A simulation study of the two-dimensional Ising case

2016

As a simplified model of a liquid nanostripe adsorbed on a chemically structured substrate surface, a two-dimensional Ising system with two boundaries at which surface fields act is studied. At the upper boundary, the surface field is uniformly negative, while at the lower boundary (a distance L apart), the surface field is negative only outside a range of extension b, where a positive surface stabilizes a droplet of the phase with positive magnetization for temperatures T exceeding the critical temperature Tw of the wetting transition of this model. We investigate the local order parameter profiles across the droplet, both in the directions parallel and perpendicular to the substrate, vary…

Surface (mathematics)Materials scienceCondensed matter physicsPINNEDCiencias FísicasOrder (ring theory)DROPLETSNanotechnology//purl.org/becyt/ford/1.3 [https]Substrate (electronics)01 natural sciences010305 fluids & plasmas//purl.org/becyt/ford/1 [https]MagnetizationWetting transitionPhase (matter)ISING0103 physical sciencesPerpendicularIsing model010306 general physicsCIENCIAS NATURALES Y EXACTASFísica de los Materiales CondensadosPhysical Review E
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Does Young's equation hold on the nanoscale? A Monte Carlo test for the binary Lennard-Jones fluid

2010

When a phase-separated binary ($A+B$) mixture is exposed to a wall, that preferentially attracts one of the components, interfaces between A-rich and B-rich domains in general meet the wall making a contact angle $\theta$. Young's equation describes this angle in terms of a balance between the $A-B$ interfacial tension $\gamma_{AB}$ and the surface tensions $\gamma_{wA}$, $\gamma_{wB}$ between, respectively, the $A$- and $B$-rich phases and the wall, $\gamma _{AB} \cos \theta =\gamma_{wA}-\gamma_{wB}$. By Monte Carlo simulations of bridges, formed by one of the components in a binary Lennard-Jones liquid, connecting the two walls of a nanoscopic slit pore, $\theta$ is estimated from the inc…

Surface (mathematics)PhysicsCondensed matter physicsStatistical Mechanics (cond-mat.stat-mech)Monte Carlo methodGeneral Physics and AstronomyThermodynamic integrationFOS: Physical sciencesComputational Physics (physics.comp-ph)Contact angleSurface tensionPhysics::Fluid DynamicsDistribution functionWetting transitionPhysics - Computational PhysicsScalingCondensed Matter - Statistical Mechanics
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Controlling the wetting properties of the Asakura-Oosawa model and applications to spherical confinement.

2012

We demonstrate for the Asakura-Oosawa model and an extension of this model that uses continuous rather than hard potentials, how wetting properties at walls can be easily controlled. By increasing the interaction range of the repulsive wall potential acting on the colloids (while keeping the polymer-wall interactions constant) polymers begin to substitute colloids at walls and the system can be driven from complete wetting of colloids via partial wetting to complete wetting of polymers. As an application, we discuss the morphology and wetting behavior of colloid-polymer mixtures in spherical confinement. We apply the recently developed 'ensemble switch method' where the Hamiltonian is exten…

chemistry.chemical_classificationMaterials sciencedigestive oral and skin physiologyNanotechnologyPolymerCondensed Matter PhysicsPhysics::Fluid DynamicsCondensed Matter::Soft Condensed MatterContact anglesymbols.namesakeColloidGibbs isothermchemistryWetting transitionChemical physicssymbolsGeneral Materials ScienceWettingHamiltonian (quantum mechanics)Interaction rangeJournal of physics. Condensed matter : an Institute of Physics journal
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