(116l) Dynamics of forced and unforced autophoretic particles

Chemically active, or autophoretic, particles that isotropically emit or absorb solute molecules undergo spontaneous self-propulsion when their activity is increased beyond a critical Péclet number (Pe). Results from numerical computations of a rigid, spherical autophoretic particle [J. Fluid Mech., 948, A41 (2022)] in unsteady rectilinear translation are presented. The particle can be freely suspended (or ‘unforced’) or subject to an external force field (or ‘forced’). The motion of an unforced particle progresses through four regimes as Pe is increased: quiescent, steady, stirring and chaos. The particle is stationary in the quiescent regime, and the solute profile is isotropic about the particle. At Pe = 4 the fore–aft symmetry in the solute profile is broken, resulting in its steady self-propulsion. the onset of self-propulsion, as has been predicted in previous studies. A further increase gives rise to the stirring regime at Pe ≈ 27, where the fluid undergoes recirculation, while the particle remains essentially stationary. As Pe is increased even further, the particle dynamics is marked by chaotic oscillations at Pe ≈ 55 and higher, which we characterize in terms of the mean square displacement and velocity autocorrelation of the particle. Our results for an autophoretic particle under a weak external force are in good agreement with asymptotic predictions [J. Fluid Mech., 916, A47 (2021)]. Additionally, we demonstrate that the strength and temporal scheduling of the external force may be tuned to modulate the chaotic dynamics at large Pe.