Non-equilibrium fluctuations and nonlinear response of an active bath

TL;DR

This study investigates how an active bath influences a passive colloidal probe's fluctuations, friction, and relaxation, revealing non-equilibrium behaviors and rheological changes consistent with recent models, and quantifying energy transfer and diffusion enhancement.

Contribution

The paper provides experimental verification of nonlinear rheology predictions for active baths, analyzing force fluctuations, viscosity changes, and energy transfer in a dense active suspension.

Findings

Active bath exhibits shear thinning at low Pe

Active bath shows shear thickening at intermediate Pe

Effective viscosity plateaus at high Pe

Abstract

We analyze the dynamics of a passive colloidal probe immersed in an active bath using an optical trap to study three physical processes: (1) the non-equilibrium fluctuations transferred to the probe by the active bath, (2) the friction experienced by the probe as it is driven through the active bath, and (3) the force relaxation of the probe returning to its equilibrium position. We measure the local force dynamics where all of the following characteristics are of $\mathcal{O}(1)$: the size of the probe colloid relative to active bath particle; the size of the probe colloid relative to the characteristic run-length of an active particle; and the timescale of probe movement to the persistence time of an active particle. We find at P\'{e}clet (Pe) $\ll 1$ the active suspension exhibits shear thinning down to the solvent viscosity (but not below); at $0.85 <$ Pe $\leq 5.1$ the active bath shear thickens; and at Pe $\geq 8.5$ the effective viscosity of the active bath shows a decreased effect of thickening and plateaus. These results are in agreement with recent modeling and simulations of the nonlinear rheology of an isotropic active bath, providing experimental verification, and suggesting the model predictions extends to moderately dense suspensions. Further, we observe that the distribution of force fluctuations depends on Pe, unlike in passive equilibrium baths. Lastly, we measure the energy transfer rate from the active bath to the probe to be $\langle J \rangle \approx 10^3$ $k_B T/$s, which leads to an increase in the effective diffusion of the probe by a factor of $\sim 2$.