AI Article Synopsis

  • The text discusses point-vortex models for generalized Euler equations, focusing on the surface quasigeostrophic (SQG) equations and the debate around finite-time singularities.
  • It highlights the use of Nambu dynamics to express point-vortex trajectories and emphasizes the geometrical interpretation of these trajectories as intersections of Hamiltonian and Casimir level sets.
  • The study reveals that in the three-point-vortex model for SQG, the collapse of solutions can occur in both self-similar and non-self-similar forms, contrasting with classical point-vortex behavior, and suggests implications for understanding singularity formation in SQG equations.

Article Abstract

Point-vortex models are presented for the generalized Euler equations, which are characterized by a fractional Laplacian relation between the active scalar and the stream function. Special focus is given to the case of the surface quasigeostrophic (SQG) equations, for which the existence of finite-time singularities is still a matter of debate. Point-vortex trajectories are expressed using Nambu dynamics. The formulation is based on a noncanonical bracket and allows for a geometrical interpretation of trajectories as intersections of level sets of the Hamiltonian and Casimir. Within this setting, we focus on the collapse of solutions for the three-point-vortex model. In particular, we show that for SQG the collapse can be either self-similar or non-self-similar. Self-similarity occurs only when the Hamiltonian is zero, while non-self-similarity appears for nonzero values of the same. For both cases, collapse is allowed for any choice of circulations within a permitted interval. These results differ strikingly from the classical point-vortex model, where collapse is self-similar for any value of the Hamiltonian, but the vortex circulations must satisfy a strict relationship. Results may also shed a light on the formation of singularities in the SQG partial differential equations, where the singularity is thought to be reached only in a self-similar way.

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http://dx.doi.org/10.1103/PhysRevE.98.023110DOI Listing

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