The curved kinetic boundary layer of active matter
arXiv:1711.01450 · doi:10.1039/C7SM01643C
Abstract
The finite reorient-time of swimmers leads to a finite run length and the kinetic accumulation boundary layer on the microscopic length scale on a non-penetrating wall. That boundary layer is the microscopic origin of the swim pressure, and is impacted by the geometry of the boundary [Yan \& Brady, \textit{J. Fluid. Mech.}, 2015, \textbf{785}, R1]. In this work we extend the analysis to analytically solve the boundary layer on an arbitrary-shaped body distorted by the local mean curvature. The solution gives the swim pressure distribution and the total force (torque) on an arbitrarily shaped body immersed in swimmers, with a general scaling of the curvature effect .
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- Transport powered by bacterial turbulence
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- Response of active Brownian particles to boundary driving
- Force renormalization for probes immersed in an active bath
- Activity-induced propulsion of a vesicle
- Kinetic temperature and pressure of an active Tonks gas
- Anisotropic swim stress in active matter with nematic order
- Forced microrheology of active colloids
- Macrotransport of active particles in periodic channels and fields: rectification and dispersion
- Passive Janus Particles Are Self-propelled in Active Nematics