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Wetting and Spreading on Patterned Surfaces
Alexandre Dupuis, Halim Kusumaatmaja, Julia Yeomans University of Oxford
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The simulations solve the hydrodynamic equations of motion for the drop.
Drop equilibrium is described by a free energy: allowing us to model surface tension and contact angles. Input parameters to the simulations are drop and substrate dimensions, surface tension, fluid density, surface tension and fluid viscosity.
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Drop spreading on a chemically striped surface: the grey and white stripes have different contact angle (click for movie)
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Experiments (J. Léopoldès and D. Bucknall) Drops on striped surfaces 1
Experiments (J.Léopoldès and D.Bucknall) Drops on striped surfaces 1. stripes narrow compared to drop radius 4. stripes of width of order drop radius 8. stripes able to contain a drop 64o / 5o
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Simulations: impact near the centre of the lyophobic stripe click for movie
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Simulations: impact near a lyophilic stripe click for movie
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The final drop shape depend on the point of impact.
Quantitative agreement between simulations and experiments Simulation vs experiments Evolution of the contact line
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Effect of the jetting velocity
Same point of impact in both simulations With an impact velocity t=0 t=10000 t=20000 t=100000 With no impact velocity
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Drop pushed gently across a chemically striped surface (click for movie)
60o /110o
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Mottle: irregular spacing of jetted drops which degrades image quality
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Drops in a square array, but with small randomness in their points of impact,
lead to mottle (click for movie)
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A drop can be confined by a hydrophobic grid – the small circle denotes the point of impact and the dark line the final drop position
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Confining a drop using a hydrophobic grid
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A hydrophobic grid prevents mottle (click for movie)
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Experiments (David Bucknall and Julien Leopoldes)
The bottom half of the substrate is patterned by hydrophobic squares
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Superhydrophobic substrates: patterning with micron-sized posts increases the contact angle of a hydrophobic surface Bico et al., Euro. Phys. Lett., 47, 220, 1999.
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A superhydrophobic surface
Mathilde Callies and David Quere 2006
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Two droplet states suspended drop: lies on top of the posts
collapsed drop: lies between the posts He et al., Langmuir, 19, 4999, 2003
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Substrate geometry qeq=110o
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Equilibrium droplets on superhydrophobic substrates
Suspended, q~160o Collapsed, q~140o On a homogeneous substrate, qeq=110o
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A drop undergoes a transition from the suspended to the
collapsed state as it evaporates (click for movie)
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Drop pushed gently across a superhydrophobic surface
collapsed suspended
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