Abstract

Stokesian Dynamics is a well-established computational method for simulating dynamics of many particles suspended in a conventional passive fluid medium such as water. Active fluids composed of self-driving microscopic particles with broken time reversal symmetry permit the emergence of a so-called odd viscosity. In this work, we extended the conventional Stokesian Dynamics formalism to incorporate the additional hydrodynamic effects due to odd viscosity under a simplified quasi-two-dimensional case. This demonstrates that Stokesian Dynamics can be generalized to simulate collective behaviors of many particles suspended in an active fluid medium with both even and odd viscosity.

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