Gravitational settling of active droplets

08 September 2022, Version 1
This content is a preprint and has not undergone peer review at the time of posting.

Abstract

The gravitational settling of oil droplets solubilizing in an aqueous micellar solution contained in a capillary channel is investigated. The motion of these active droplets reflects a competition between gravitational and Marangoni forces, the latter due to interfacial tension gradients generated by differences in filled- micelle concentrations along the oil-water interface. This competition is studied by varying the surfactant concentration, the density difference between the droplet and the continuous phase, and the viscosity of the continuous phase. The Marangoni force enhances the settling speed of an active droplet when compared to the Hadamard-Rybczynski prediction for a (surfactant free) droplet settling in Stokes flow. The Marangoni force can also induce lateral droplet motion, suggesting that the Marangoni and gravitational forces are not always aligned. The decorrelation rate (š¯›¼) of the droplet motion, measured as the initial slope of the velocity autocorrelation and indicative of the extent to which the Marangoni and gravitational forces are aligned during settling, is examined as a function of the droplet size: correlated motion (small values of š¯›¼) is observed at both small and large droplet radii, whereas significant decorrelation can occur between these limits. This behavior of active droplets settling in a capillary channel is in marked contrast to that observed in a dish, where the decorrelation rate increases with the droplet radius before saturating at large values of droplet radius. A simple relation for the crossover radius at which the maximal value of š¯›¼ occurs for an active settling droplet is proposed.

Keywords

droplets
active matter

Supplementary materials

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Supplementary Material
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Contains additional details on the experimental methods, data analysis techniques, and material properties of the various systems used in the main paper.
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Video S1
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Bromodecane droplet of R = 41 Ī¼m moving through a solution of 3 wt% Triton X-100 on a glass bottom dish.
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Video S2
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Bromodecane droplet of R = 71 Ī¼m moving through a solution of 3 wt% Triton X-100 on a glass bottom dish. Video taken at 20 fps on a Nikon Eclipse Ts2 microscope using an Imaging Source DFK 23UX249 color camera and IC Capture at 4x magnification (Nikon objective) (see experimental methods for details). Video shown in real time.
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Video S3
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Bromodecane droplet of R = 41 Ī¼m settling through a solution of 3 wt% Triton X-100. Video taken at 40 fps using a PCO Panda sCMOS camera and Ī¼Manager software on a custom- built side-imaging microscope using a Nikon 2x objective (see experimental methods for details). Video shown in real time.
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Video S4
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Video S4: Bromodecane droplet of R = 73 Ī¼m settling through a solution of 3 wt% Triton X-100. Video taken at 40 fps using a PCO Panda sCMOS camera and Ī¼Manager software on a custom- built side-imaging microscope using a Nikon 2x objective (see experimental methods for details). Video shown in real time.
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Video S5
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Bromodecane droplet of R = 49 Ī¼m settling through a solution of 4.75 wt% Triton X- 100 with 5 wt% poly(ethylene glycol) (MW=20,000 g/mol). Video taken at 40 fps using a PCO Panda sCMOS camera and Ī¼Manager software on a custom-built side-imaging microscope using a Nikon 10x objective (see experimental methods for details). Image brightness and contrast adjusted to better visualize droplet trail using ImageJ. Video shown in real time.
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Video S6
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Bromodecane droplet of R = 69 Ī¼m settling through a solution of 4.75 wt% Triton X- 100 with 5 wt% poly(ethylene glycol) (MW=20,000 g/mol). Video taken at 40 fps using a PCO Panda sCMOS camera and Ī¼Manager software on a custom-built side-imaging microscope using a Nikon 10x objective (see experimental methods for details). Image brightness and contrast adjusted to better visualize droplet trail using ImageJ. Video shown in real time.
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