Abstract

In recent decades novel solid substrates have been designed which change their wettability in response to light or an electrostatic field. Here, we investigate a droplet on substrates with oscillating uniform wettability by varying minimum and maximum contact angles and frequency. To simulate this situation, we use our previous work [Grawitter and Stark, Soft Matter, 2021, 17, 2454], where we implemented the boundary element method in combination with the Cox-Voinov law for the contact-line velocity, to determine the fluid flow inside a droplet. After a transient regime the droplet performs steady oscillations, the amplitude of which decreases with increasing frequency. For slow oscillations our numerical results agree well with the linearized spherical-cap model. They collapse on a master curve when we rescale frequency by a characteristic relaxation time. In contrast, for fast oscillations we observe significant deviations from the master curve. The decay of the susceptibility is weaker and the phase shift between oscillations in wettability and contact angle stays below the predicted π/2. The reason becomes obvious when studying the combined dynamics of droplet height and contact angle. It reveals non-reciprocal shape changes during one oscillation period even at low frequencies due to the induced fluid flow inside the droplet, which are not captured by the spherical-cap model. Similar periodic non-reciprocal shape changes occur at low frequencies when the droplet is placed on an oscillating nonuniform wettability profile with six-fold symmetry. Such profiles are inspired by the light intensity pattern of Laguerre-Gauss laser modes. Since the non-reciprocal shape changes induce fluid circulation, which is controllable from the outside, our findings envisage the design of targeted microfluidic transport of solutes inside the droplet.

Highlights

  • The shape a liquid droplet forms on a flat surface is determined by the wettability landscape of the surface

  • We consider a droplet on a substrate, where the uniform wettability expressed by the equilibrium contact angle yeq(t) oscillates with a frequency f between a minimum and maximum value: yeq(t) = ym eqin +Ásin2(pft)

  • We have studied liquid droplets on substrates with oscillating wettability focussing on their shape and internal fluid flow

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Summary

Introduction

The shape a liquid droplet forms on a flat surface is determined by the wettability landscape of the surface. One uses a thin-film equation to evaluate the droplet dynamics via its height profile,[31,32,33,34] which means the contact angle should be small and cannot exceed 90 degrees Another approach, which we will discuss in detail below, is the spherical cap model. We find that the contact angle oscillations of the droplet decrease with increasing frequency For slow oscillations this can be well described by the spherical-cap model, which even provides a characteristic time scale to map the oscillations onto a common master curve.

Simulation method
Stokes flow
Boundary conditions
Boundary element method
Droplet on a substrate of oscillating uniform wettability
Phenomenology
Deformation and pumping
Oscillations of nonuniform wettability profiles
Conclusions
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