Calculation of nanodrop profile from fluid density distribution
| Autor: | Gersh O. Berim, Eli Ruckenstein |
|---|---|
| Rok vydání: | 2016 |
| Předmět: |
Imagination
Chemistry Drop (liquid) media_common.quotation_subject Nanotechnology 02 engineering and technology Surfaces and Interfaces Radial line Mechanics 010402 general chemistry 021001 nanoscience & nanotechnology 01 natural sciences Potential energy 0104 chemical sciences Physics::Fluid Dynamics Contact angle Colloid and Surface Chemistry Density functional theory Surface layer Wetting Physical and Theoretical Chemistry 0210 nano-technology media_common |
| Zdroj: | Advances in Colloid and Interface Science. 231:15-22 |
| ISSN: | 0001-8686 |
| DOI: | 10.1016/j.cis.2016.02.004 |
| Popis: | Two approaches are examined, which can be used to determine the drop profile from the fluid density distributions (FDDs) obtained on the basis of microscopic theories. For simplicity, only two-dimensional (cylindrical, or axisymmetrical) distributions are examined and it is assumed that the fluid is either in contact with a smooth solid or separated from the smooth solid by a lubricating liquid film. The first approach is based on the sharp-kink interface approximation in which the density of the liquid inside and the density of the vapor outside the drop are constant with the exception of the surface layer of the drop where the density is different from the above ones. In this case, the drop profile was calculated by minimizing the total potential energy of the system. The second approach is based on a nonuniform FDD obtained either by the density functional theory or molecular dynamics simulations. To determine the drop profile from such an FDD, which does not contain sharp interfaces, three procedures can be used. In the first two procedures, P1 and P2, the one-dimensional FDDs along straight lines which are parallel to the surface of the solid are extracted from the two-dimensional FDD. Each of those one-dimensional FDDs has a vapor-liquid interface at which the fluid density changes from vapor-like to liquid-like values. Procedure P1 uses the locations of the equimolar dividing surfaces for the one-dimensional FDDs as points of the drop profile. Procedure P2 is based on the assumption that the fluid density is constant on the surface of the drop, that density being selected either arbitrarily or as a fluid density at the location of the equimolar dividing surface for one of the one-dimensional FDDs employed in procedure P1. In the third procedure, P3, which is suggested for the first time in this paper, the one-dimensional FDDs are taken along the straight lines passing through a selected point inside the drop (radial line). Then, the drop profile is calculated like in procedure P1. It is shown, that procedure P3 provides a drop profile which is more reasonable than the other ones. Relationship of the discussed procedures to those used in image analysis is briefly discussed. |
| Databáze: | OpenAIRE |
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