Abstract

The stationary-state distribution function of confined active Brownian particles (ABPs) is analyzed by computer simulations and analytical calculations. We consider a radial harmonic as well as an anharmonic confinement potential. In the simulations, the ABP is propelled with a prescribed velocity along a body-fixed direction, which is changing in a diffusive manner. For the analytical approach, the Cartesian components of the propulsion velocity are assumed to change independently; active Ornstein–Uhlenbeck particle (AOUP). This results in very different velocity distribution functions. The analytical solution of the Fokker–Planck equation for an AOUP in a harmonic potential is presented and a conditional distribution function is provided for the radial particle distribution at a given magnitude of the propulsion velocity. This conditional probability distribution facilitates the description of the coupling of the spatial coordinate and propulsion, which yields activity-induced accumulation of particles. For the anharmonic potential, a probability distribution function is derived within the unified colored noise approximation. The comparison of the simulation results with theoretical predictions yields good agreement for large rotational diffusion coefficients, e.g. due to tumbling, even for large propulsion velocities (Péclet numbers). However, we find significant deviations already for moderate Péclet number, when the rotational diffusion coefficient is on the order of the thermal one.

Highlights

  • The distinct feature of active systems is their autonomous motion powered by an internal energy source or by utilizing energy from their environment [1,2,3,4,5,6,7,8,9]

  • We have investigated the properties of active Brownian particle (ABP) confined in a radially symmetric potential

  • The study of ABPs and active Ornstein– Uhlenbeck particle (AOUP) confined in a harmonic potential clearly reveals the strong effect of the condition ∣v∣ = v0 = const. on the stationary-state properties

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Summary

January 2018

This results in very different velocity distribution functions. The analytical solution of the Fokker–Planck equation for an AOUP in a harmonic potential is presented and a conditional distribution function is provided for the radial particle distribution at a given magnitude of the propulsion velocity. This conditional probability distribution facilitates the description of the coupling of the spatial coordinate and propulsion, which yields activity-induced accumulation of particles. The comparison of the simulation results with theoretical predictions yields good agreement for large rotational diffusion coefficients, e.g. due to tumbling, even for large propulsion velocities (Péclet numbers).

Introduction
Active Brownian particle
Active Ornstein–Uhlenbeck particle
AOUP in harmonic potential
22 Lrv v0 r exp
One-dimensional system
Unified colored noise approximation
UCNA distribution function of radial potential
Z0 exp
Comparison of simulation and UCNA results for anharmonic potential
Comparison of AOUP simulations with UCNA
Comparison of ABP simulations and UCNA
Summary and conclusions
Full Text
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