Maximum Spreading and Rebound of a Droplet Impacting onto a

Apr 10, 2018 - ... Reynolds number impact of droplets onto hydrophobic or superhydrophobic spherical solid surfaces. The Supporting Information is ava...
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Maximum Spreading and Rebound of a Droplet Impacting onto a Spherical Surface at low Weber numbers Alireza Bordbar, Arsalan Taassob, Danial Khojasteh, Marco Marengo, and Reza Kamali Langmuir, Just Accepted Manuscript • DOI: 10.1021/acs.langmuir.8b00625 • Publication Date (Web): 10 Apr 2018 Downloaded from http://pubs.acs.org on April 10, 2018

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Maximum Spreading and Rebound of a Droplet Impacting onto a Spherical Surface at low Weber numbers Alireza Bordbara, Arsalan Taassoba, Danial Khojasteha,b, Marco Marengoc, Reza Kamalia* a

b

School of Mechanical Engineering, Shiraz University, Shiraz, 71936-16548, Iran

School of Civil & Environmental Engineering, UNSW Water Research Laboratory, 110 King St, Manly Vale, NSW 2093, Australia

c

School of Computing, Engineering and Mathematics, University of Brighton, BN2 4GJ Brighton, United Kingdom

Abstract The spreading and rebound patterns of low-viscous droplets upon impacting spherical solid surfaces are investigated numerically. The studied cases consider a droplet impinging onto hydrophobic and superhydrophobic surfaces with various parameters varied throughout the study and their effects on the post-impingement behavior are discussed. These parameters include impact Weber number (through varying the surface tension and impingement velocity), the size ratio of the droplet to the solid surface, and the surface contact angle. According to the findings, the maximum spreading diameter increases with the impact velocity, with an increase of the sphere diameter, with a lower surface wettability and a lower surface tension. Typical outcomes of the impact include 1) complete rebound, 2) splash, and 3) a final deposition stage after a series of spreading and recoiling phases. Finally, a novel, practical model is proposed, which can reasonably predict the maximum deformation of low Reynolds number impact of droplets onto hydrophobic or superhydrophobic spherical solid surfaces.

*

Corresponding author: [email protected]

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Keywords: Droplet impact, Hydrophobicity, Curved surfaces, Droplet rebound, Spreading diameter, CFD. 1. Introduction Droplet impact onto solid surfaces is a phenomenon frequently observed in both nature and engineering applications.1 Common examples include impact onto plant leaves,2 internal combustion engines where fuel droplets interact with piston and liner walls,3 inkjet printing,4 droplet-based microfluidics,5 anti-icing,6 spray cooling,7,8 crude oil industry, etc. There are also many applications in chemical and petroleum processing, such as fluid catalytic cracking (FCC) where atomized droplets are brought into contact with high temperature fluidized catalyst particles.9 Depending on the conditions of impact, occurrence of different phenomena, such as spreading, bouncing or splashing is possible.10 The determining factors for the post-impingement behavior are droplet size, impact velocity and direction, liquid properties (e.g. density, viscosity, and viscoelasticity), solid surface properties (e.g. roughness and wettability), surface or interfacial tension, and substrate geometry.11,12 These effects are best described and assessed when appropriate dimensionless groups are used. Weber (We) and Reynolds (Re) numbers are mostly employed in this regard. Weber number represents the ratio of kinetic energy to surface energy (

  

) and is a measure of the deformability of the droplet; and Re number is the ratio of   13 ). 

inertia to viscosity effect (

In terms of wettability, the solid substrate is either hydrophilic (wettable) or hydrophobic (nonwettable). Hydrophobic surfaces (HS) and superhydrophobic surfaces (SHS) possess some unique and practical properties such as surface cleaning,14 anti-fouling, anti-icing, dropwise condensation15 and drag reduction.16 A superhydrophobic surface (SHS) is standardly defined as 2 ACS Paragon Plus Environment

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a surface with an equilibrium contact angle (CA) greater than 150˚ and very low (