Weak and Strong Solutions to the Forced Fractional Euler Alignment System

Abstract

We consider a hydrodynamic model of self-organized evolution of agents, with singular interaction kernel ${\varphi }_{\alpha }(x)=1/|x{|}^{1+\alpha }$ ($0<\alpha <2$), in the presence of an additional external force. Well-posedness results are already available for the unforced system in classical regularity spaces. We define a notion of solution in larger function spaces, in particular in $L^{\infty }$ ("weak solutions") and in $W^{1,\infty }$ ("strong solutions"), and we discuss existence and uniqueness of these solutions. Furthermore, we show that several important properties of classical solutions carry over to these less regular ones. In particular, we give Onsager-type criteria for the validity of the natural energy law for weak solutions of the system, and we show that fast alignment (weak and strong solutions) and flocking (strong solutions) still occur in the forceless case.

arXiv comment36 pages

References in corpus (9)

• Global well-posedness for the critical 2D dissipative quasi-geostrophic equation
• A new model for self-organized dynamics and its flocking behavior
• Critical thresholds in flocking hydrodynamics\\with nonlocal alignment
• Global regularity for the fractional Euler alignment system
• Eulerian dynamics with a commutator forcing III. Fractional diffusion of order $0<\alpha <1$
• Global existence and stability of nearly aligned flocks
• Critical thresholds in 1D Euler equations with nonlocal forces
• Eulerian dynamics with a commutator forcing
• Global regularity for 1D Eulerian dynamics with singular interaction forces