Towards a quantitative kinetic theory of polar active matter
arXiv:1401.8056 · doi:10.1140/epjst/e2014-02192-0
Abstract
A recent kinetic approach for Vicsek-like models of active particles is reviewed. The theory is based on an exact Chapman-Kolmogorov equation in phase space. It can handle discrete time dynamics and "exotic" multi-particle interactions. A nonlocal mean-field theory for the one-particle distribution function is obtained by assuming molecular chaos. The Boltzmann approach of Bertin et al., Phys. Rev. E 74, 022101 (2006) and J. Phys. A: Math. Theor. 42, 445001 (2009), is critically assessed and compared to the current approach. In Boltzmann theory, a collision starts when two particles enter each others action spheres and is finished when their distance exceeds the interaction radius. The average duration of such a collision, , is measured for the Vicsek model with continuous time-evolution. If the noise is chosen to be close to the flocking threshold, the average time between collisions is found to be roughly equal to at low densities. Thus, the continuous-time Vicsek-model near the flocking threshold cannot be accurately described by a Boltzmann equation, even at very small density because collisions take so long that typically other particles join in, rendering Boltzmann's binary collision assumption invalid. Hydrodynamic equations for the phase space approach are derived by means of a Chapman-Enskog expansion. The equations are compared to the Toner-Tu theory of polar active matter. New terms, absent in the Toner-Tu theory, are highlighted. Convergence problems of Chapman-Enskog and similar gradient expansions are discussed.
References in corpus (9)
- Novel type of phase transition in a system of self-driven particles
- Collective motion of self-propelled particles interacting without cohesion
- Hydrodynamic equations for self-propelled particles: microscopic derivation and stability analysis
- Spontaneously ordered motion of self-propelled particles
- New aspects of the continuous phase transition in the scalar noise model (SNM) of collective motion
- Cluster dynamics and cluster size distributions in systems of self-propelled particles
- Phase transitions in swarming systems: A recent debate
- Kinetic theory for systems of self-propelled particles with metric-free interactions
- Thermal fluctuations in the lattice Boltzmann method for non-ideal fluids
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- Exact Hydrodynamic Description of Active Lattice Gases
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- Active matter beyond mean-field: Ring-kinetic theory for self-propelled particles
- Polar active liquids: a universal classification rooted in nonconservation of momentum
- Large density expansion of a hydrodynamic theory for self-propelled particles
- The BBGKY Hierarchy and Fokker-Planck Equation for Many-Body Dissipative Randomly Driven Systems
- Order-disorder transition in repulsive self-propelled particle systems
- Comment on Ihle, "Towards a quantitative kinetic theory of polar active matter"
- Discussion on Peshkov et al., "Boltzmann-Ginzburg-Landau approach for continuous descriptions of generic Vicsek-like models"
- Transport coefficients of self-propelled particles. II. Numerics for vorticity fluctuations and the reverse perturbation method
- Transport coefficients of self-propelled particles: Reverse perturbations and transverse current correlations
- Reply to comment on "Towards a quantitative kinetic theory of polar active matter" by Bertin et al
- Discussion on Ohta et al., "Traveling bands in self-propelled soft particles"
- Gaussian theory for spatially distributed self-propelled particles
- Kinetic theory of decentralized learning for smart active matter
- Reduced description method in the kinetic theory of Brownian motion with active fluctuations