Inertia drives a flocking phase transition in viscous active fluids
arXiv:1907.03492 · doi:10.1103/PhysRevX.11.031063
Abstract
How fast must an oriented collection of extensile swimmers swim to escape the instability of viscous active suspensions? We show that the answer lies in the dimensionless combination , where is the suspension mass density, the swim speed and the active stress. Linear stability analysis shows that for small disturbances grow at a rate linear in their wavenumber , and that the dominant instability mode involves twist. The resulting steady state in our numerical studies is isotropic hedgehog-defect turbulence. Past a first threshold of order unity we find a slower growth rate, of ; the numerically observed steady state is {\it phase-turbulent}: noisy but {\it aligned} on average. We present numerical evidence in three and two dimensions that this inertia driven flocking transition is continuous, with a correlation length that grows on approaching the transition. For much larger we find an aligned state linearly stable to perturbations at all . Our predictions should be testable in suspensions of mesoscale swimmers [D Klotsa, Soft Matter \textbf{15}, 8946 (2019)].
arXiv commentVersion of the manuscript accepted in PRX
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