Abstract

In real life, sessile droplets usually have a three-dimensional shape, making it difficult to understand their forced wetting behavior, both from an experimental and a theoretical perspective. Even in the case of spreading under quasi-static conditions, where the droplet shape is described by the Young–Laplace equation, there is no fundamental approach to describe the contact line evolution. In the present work, a few existing approaches on this issue are analyzed and assessed. It is shown that an experimentally inspired fixed shape for the contact line of droplets that are spreading under the action of tangential forces can be considered equivalent to a theory for contact line motion. There is a lack of experimental data for contact line evolution under arbitrary scenarios of forces. Such data will be very helpful for the further development of the suggested approach to contact line motion. Of particular interest is the case of small contact angle droplets, for which a top view can clearly indicate the contact line location. On the contrary, in such droplets, the direct experimental measurement of contact angle profile is very difficult. This must be estimated theoretically; thus, a special approach has been developed here for this purpose.

Highlights

  • The process of wetting of a solid substrate by a liquid is of paramount importance in several industrial processes [1]

  • The usual approach is to present the contact angle distribution with respect to the so-called azimuthal angle but, instead, we found it more fruitful to use the contact line length starting from the rear edge of the droplet for this purpose

  • Spreading begins and the contact line shape becomes a function of the tangential force BoT. This shape is completely parameterized through Equation (6), and the evolution problem is transformed to seeking of the b value that leads, through the procedure described in Appendix B, to a maximum contact angle equal to φA

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Summary

Introduction

The process of wetting of a solid substrate by a liquid is of paramount importance in several industrial processes [1]. Further from the contact angle profile, a complete model of the contact line evolution during application of a tangential force to a droplet was proposed in [13], based exclusively on experimental data. On the basis of these results, it is shown that ellipsis is not an acceptable shape for the contact line under tangential force.

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