Marangoni flow at droplet interfaces: Three-dimensional solution and applications
By M. Schmitt, Holger Stark. 2015
148 citations recorded by the source corpus.
The Marangoni effect refers to fluid flow induced by a gradient in surface tension at a fluid-fluid interface. We determine the full three-dimensional Marangoni flow generated by a non-uniform surface tension profile at the interface of a self-propelled spherical emulsion droplet. For all flow fields inside, outside, and at the interface of the droplet, we give analytical formulas. We also calculate the droplet velocity vector $\mathbf{v}^D$, which describes the swimming kinematics of the droplet, and generalize the squirmer parameter $\beta$, which distinguishes between different swimmer types called neutral, pusher, or puller. In the second part of this paper, we present two illustrative examples, where the Marangoni effect is used in active emulsion droplets. First, we demonstrate how micelle adsorption can spontaneously break the isotropic symmetry of an initially surfactant-free emulsion droplet, which then performs directed motion. Second, we think about light-switchable surfactants and laser light to create a patch with a different surfactant type at the droplet interface. Depending on the setup such as the wavelength of the laser light and the surfactant type in the outer bulk fluid, one can either push droplets along unstable trajectories or pull them along straight or oscillatory trajectories regulated by specific parameters. We explore these cases for strongly absorbing and for transparent droplets.
Subfields: Biomedical Engineering, Condensed Matter Physics, Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/6e806f54df3210ad2e65fff2f3d4d916bb668e3f
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Citations in the corpus
- Self-Propulsion of Chemically Active Droplets (2022, methodology): “…surface concentration of pristine surfactant (Thutupalli et al. 2011, Schmitt & Stark 2013) with the convecting surface flow obtained by solving Stokes’ equations inside and outside the droplet in linear response to the Marangoni forcing (Morozov & Michelin 2019a, Schmitt & Stark 2013, 2016).”