Incompressible active phases at an interface. I. Formulation and axisymmetric odd flows

TL;DR

This paper formulates the free-boundary dynamics of a 2D chiral active monolayer droplet on a 3D fluid, providing exact solutions for axisymmetric cases and exploring effects like Hall viscosity on droplet behavior.

Contribution

It introduces a mathematical framework for axisymmetric chiral active monolayer droplets, including exact solutions and analysis of Hall viscosity effects, advancing understanding of active fluid interfaces.

Findings

Exact solutions for axisymmetric chiral surface flows.

Velocity field varies from solid-body rotation to edge currents.

Hall viscosity influences radial and transverse flow coupling.

Abstract

Inspired by the recent realization of a 2D chiral fluid as an active monolayer droplet moving atop a 3D Stokesian fluid, we formulate mathematically its free-boundary dynamics. The surface droplet is described as a general 2D linear, incompressible, and isotropic fluid, having a viscous shear stress, an active chiral driving stress, and a Hall stress allowed by the lack of time-reversal symmetry. The droplet interacts with itself through its driven internal mechanics and by driving flows in the underlying 3D Stokes phase. We pose the dynamics as the solution to a singular integral-differential equation, over the droplet surface, using the mapping from surface stress to surface velocity for the 3D Stokes equations. Specializing to the case of axisymmetric droplets, exact representations for the chiral surface flow are given in terms of solutions to a singular integral equation, solved using both analytical and numerical techniques. For a disc-shaped monolayer, we additionally employ a semi-analytical solution that hinges on an orthogonal basis of Bessel functions and allows for efficient computation of the monolayer velocity field, which ranges from a nearly solid-body rotation to a unidirectional edge current depending on the subphase depth and the Saffman-Delbruck length. Except in the near-wall limit, these solutions have divergent surface shear stresses at droplet boundaries, a signature of systems with codimension one domains embedded in a three-dimensional medium. We further investigate the effect of a Hall viscosity, which couples radial and transverse surface velocity components, on the dynamics of a closing cavity.