Splashing of droplets impacting superhydrophobic substrates
A drop of radius R impacting a superhydrophobic substrate at a velocity V keeps its integrity and spreads over the solid for V < Vc or splashes, disintegrating into tiny droplets violently ejected radially outwards for V Vc, with Vc the critical velocity for splashing. In contrast with the case o...
| Autores: | , , |
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| Tipo de recurso: | artículo |
| Estado: | Versión aceptada para publicación |
| Fecha de publicación: | 2019 |
| País: | España |
| Institución: | Universidad de Sevilla (US) |
| Repositorio: | idUS. Depósito de Investigación de la Universidad de Sevilla |
| OAI Identifier: | oai:idus.us.es:11441/159223 |
| Acceso en línea: | https://hdl.handle.net/11441/159223 https://doi.org/10.1017/jfm.2019.258 |
| Access Level: | acceso abierto |
| Palabra clave: | Breakup/coalescence Drops |
| Sumario: | A drop of radius R impacting a superhydrophobic substrate at a velocity V keeps its integrity and spreads over the solid for V < Vc or splashes, disintegrating into tiny droplets violently ejected radially outwards for V Vc, with Vc the critical velocity for splashing. In contrast with the case of drop impact onto a partially wetting substrate, Riboux & Gordillo [Phys. Rev. Lett. 113, 024507 (2014)], our experiments reveal that the critical condition for the splashing of water droplets impacting a superhydrophobic substrate at normal atmospheric conditions is characterized by a value of the critical Weber number, Wec = ρV2 cR/σ ∼ O(100), which hardly depends on the Ohnesorge number Oh = µ/√ρRσ and is noticeably smaller than the corresponding value for the case of partially wetting substrates. Here we present a self-consistent model, in very good agreement with experiments, capable to predict Wec as well as the full dynamics of the drop expansion and disintegration for We Wec. In particular, our model is able to accurately predict the time evolution of the position of the rim bordering the expanding lamella for We 20 as well as the diameters and velocities of the small and fast droplets ejected when We Wec. |
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