Abstract

We propose a coupled system for the interaction between Cucker-Smaleflocking particles and viscous compressible fluids, and present aglobal existence theory and time-asymptotic behavior for theproposed model in the spatial periodic domain $\mathbb{T}^3$. Our modelconsists of the kinetic Cucker-Smale model for flocking particlesand the isentropic compressible Navier-Stokes equations for fluids,and these two models are coupled through a drag force, which is responsible for the asymptotic alignmentbetween particles and fluid. For the asymptotic flocking behavior,we explicitly construct a Lyapunov functional measuring thedeviation from the asymptotic flocking states. For a large viscosityand small initial data, we show that the velocities of Cucker-Smaleparticles and fluids are asymptotically aligned to the commonvelocity.

Highlights

  • Collective behavior is a common natural phenomenon, such as fish swimming, birds flocking and agents synchronizing

  • It is expected that the developed technique as well as the physical discoveries could be potentially useful for designing automatic controllers, e.g. deep brain stimulators, to remedy some synchronization-induced mental disorders including Parkinson disease and epilepsy

  • In this report, we investigate the multi-cluster flocking behavior of the hierarchical Cucker-Smale model parameterized by a constant $\beta$ measuring the strength of the interaction between agents

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Summary

Introduction

Collective behavior is a common natural phenomenon, such as fish swimming, birds flocking and agents synchronizing. Hyeong-Ohk Bae Department of Financial Engineering,Ajou University, Suwon 443-749, Korea Abstract: We propose a coupled system for the interaction between CuckerSmale flocking particles and viscous compressible fluids, and present a global existence theory and time-asymptotic behavior for the proposed model in the spatial periodic domain T^3 . For a large viscosity and small initial data, we show that the velocities of Cucker-Smale particles and fluids are asymptotically aligned to the common velocity.

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