Spherical Droplet Deposition—Mechanistic Model

In the currently existing physical models of wetting a solid substrate by a liquid drop, the contact angle is determined on the basis of the equilibrium of forces acting tangentially to the wetted surface at any point in the perimeter of the wetted area, ignoring the forces (or their components) act...

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Main Authors: Jacek A. Michalski, Slawomir Jakiela
Format: Article
Language:English
Published: MDPI AG 2021-02-01
Series:Coatings
Subjects:
Online Access:https://www.mdpi.com/2079-6412/11/2/248
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spelling doaj-f2681341137c4791a8cff464e01ac7db2021-02-20T00:02:36ZengMDPI AGCoatings2079-64122021-02-011124824810.3390/coatings11020248Spherical Droplet Deposition—Mechanistic ModelJacek A. Michalski0Slawomir Jakiela1Faculty of Civil Engineering, Mechanics and Petrochemistry, Institute of Chemistry, Warsaw University of Technology, Ignacego Lukasiewicza 17, 09-400 Plock, PolandDepartment of Physics and Biophysics, Institute of Biology, Warsaw University of Life Sciences, Nowoursynowska 159, Building 34, 02-776 Warsaw, PolandIn the currently existing physical models of wetting a solid substrate by a liquid drop, the contact angle is determined on the basis of the equilibrium of forces acting tangentially to the wetted surface at any point in the perimeter of the wetted area, ignoring the forces (or their components) acting perpendicular to this area. In the solution shown in the paper, the equilibrium state of forces acting on a droplet was determined based on the minimum mechanical energy that the droplet achieves in the state of equilibrium. This approach allows one to take into account in the model, in addition to the forces tangential to the wetted surface, also forces perpendicular to it (also the force of adhesion), moreover, these may be dispersed forces acting on the entire interface, not on a single point. The correctness of this approach is confirmed by the derived equations concerning the forces acting on the liquid both tangentially and perpendicularly to the wetted surface. The paper also identifies the areas of solutions in which the obtained equilibrium of forces is stable and areas of unstable equilibrium of forces. The solution is formulated both for isothermal and isochoric system. Based on the experimental data accessible in the literature, the condition that has to be met by the droplets (and their surroundings) during measurements performed under gravity conditions was formulated.https://www.mdpi.com/2079-6412/11/2/248contact anglesessile dropletspherical dropletwetting
collection DOAJ
language English
format Article
sources DOAJ
author Jacek A. Michalski
Slawomir Jakiela
spellingShingle Jacek A. Michalski
Slawomir Jakiela
Spherical Droplet Deposition—Mechanistic Model
Coatings
contact angle
sessile droplet
spherical droplet
wetting
author_facet Jacek A. Michalski
Slawomir Jakiela
author_sort Jacek A. Michalski
title Spherical Droplet Deposition—Mechanistic Model
title_short Spherical Droplet Deposition—Mechanistic Model
title_full Spherical Droplet Deposition—Mechanistic Model
title_fullStr Spherical Droplet Deposition—Mechanistic Model
title_full_unstemmed Spherical Droplet Deposition—Mechanistic Model
title_sort spherical droplet deposition—mechanistic model
publisher MDPI AG
series Coatings
issn 2079-6412
publishDate 2021-02-01
description In the currently existing physical models of wetting a solid substrate by a liquid drop, the contact angle is determined on the basis of the equilibrium of forces acting tangentially to the wetted surface at any point in the perimeter of the wetted area, ignoring the forces (or their components) acting perpendicular to this area. In the solution shown in the paper, the equilibrium state of forces acting on a droplet was determined based on the minimum mechanical energy that the droplet achieves in the state of equilibrium. This approach allows one to take into account in the model, in addition to the forces tangential to the wetted surface, also forces perpendicular to it (also the force of adhesion), moreover, these may be dispersed forces acting on the entire interface, not on a single point. The correctness of this approach is confirmed by the derived equations concerning the forces acting on the liquid both tangentially and perpendicularly to the wetted surface. The paper also identifies the areas of solutions in which the obtained equilibrium of forces is stable and areas of unstable equilibrium of forces. The solution is formulated both for isothermal and isochoric system. Based on the experimental data accessible in the literature, the condition that has to be met by the droplets (and their surroundings) during measurements performed under gravity conditions was formulated.
topic contact angle
sessile droplet
spherical droplet
wetting
url https://www.mdpi.com/2079-6412/11/2/248
work_keys_str_mv AT jacekamichalski sphericaldropletdepositionmechanisticmodel
AT slawomirjakiela sphericaldropletdepositionmechanisticmodel
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