Abstract

We study theoretically an active colloid whose polar axis of self-propulsion rotates to point parallel (antiparallel) to an imposed chemical gradient. We show that the coupling of this ‘chemotactic’ (‘antichemotactic’) response to phoretic translational motion yields remarkable two-particle dynamics reflecting the non-central and non-reciprocal character of the interaction. A pair of mutually chemotactic colloids trap each other in a final state of fixed separation resulting in a self-propelled active dimer. A second type of bound state is observed when the polar axes undergo periodic cycles leading to phase-locked circular motion around a common centre. A pair of swimmers with mismatched phoretic mobilities execute a dance in which they twirl around one another while moving jointly in a wide circle. For sufficiently small initial separation, the speed of self-propulsion controls the transition from bound to scattering states. Mutually anti-chemotactic swimmers always scatter apart. For the special case in which one of the two colloids has uniform surface activity we succeed in exactly classifying the fixed points underlying the bound states, and identify the bifurcations leading to transitions from one type of bound state to another. The varied dynamical behaviours are accessible by tuning the swimmer design and are summarised in state diagrams.

Highlights

  • Gradients in the concentration of a solute along the surface of a particle in a fluid produce pressure differences, and a slip flow, parallel to the surface

  • We have explored theoretically the varieties of dynamics exhibited by polar self-diffusiophoretic colloids, focusing on the case where the motion is planar

  • Gradients in the diffusing chemical species—generated by other colloids—affect the motion of the colloids, directly by translating them, and indirectly by rotating their polar axes and their self-propelling velocities. These effects cooperate and compete, with remarkable dynamical consequences ranging from trapping, scattering and simple orbits around a fixed source to complex pairs of dances, which are the main results presented in this paper

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Summary

11 June 2019

Original content from this work may be used under the terms of the Creative Abstract. This work must maintain attribution to the (‘antichemotactic’) response to phoretic translational motion yields remarkable two-particle author(s) and the title of dynamics reflecting the non-central and non-reciprocal character of the interaction. Mutually chemotactic colloids trap each other in a final state of fixed separation resulting in a selfpropelled active dimer. A second type of bound state is observed when the polar axes undergo periodic cycles leading to phase-locked circular motion around a common centre. For sufficiently small initial separation, the speed of self-propulsion controls the transition from bound to scattering states. For the special case in which one of the two colloids has uniform surface activity we succeed in exactly classifying the fixed points underlying the bound states, and identify the bifurcations leading to transitions from one type of bound state to another. The varied dynamical behaviours are accessible by tuning the swimmer design and are summarised in state diagrams

Introduction
Interacting active colloids
Single active colloid near a source of product molecules
Bound final state
Orbits
Two mobile swimmers
Binary swimmers
Conclusions
Full Text
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