Abstract

Here we characterize the motility of athermal swimming droplets within the framework of active rotational diffusion. Just like active colloids, their trajectories can be modeled with a constant velocity VV and a slow angular diffusion, but the random changes in direction are not thermally driven. Instead, VV is determined by the interfacial tension gradient along the droplet surface, while local micellar fluctuations lead to droplet reorientation with a persistence time ττ. We show that the origin of locomotion is the difference in the critical micellar concentration ΔΔCMC in the front and the back of the droplet. Tuning this parameter by salt controls VV from 3−153-15 diameters d/sd/s. Surfactant concentration has little effect on speed, but leads to a dramatic decrease in ττ over four orders of magnitude. The corresponding range of the effective diffusion constant DeD_e extends beyond the realm of synthetic or living swimmers, in which VV is limited by fuel consumption and ττ is set by temperature or biological activity, respectively. Our tunable swimmers are ideal candidates for the study of the departure from equilibrium to high levels of activity, on both the single particle level and their collective behavior, including the motility-induced phase separation (MIPS).

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