English

Stability of the Inviscid Power-Law Vortex

Analysis of PDEs 2026-02-04 v4 Fluid Dynamics

Abstract

We prove that the power-law vortex ω(x)=βxα\overline{\omega}(x) = \beta |x|^{-\alpha}, which explicitly solves the stationary unforced incompressible Euler equations in R2\mathbb{R}^2 in both physical and self-similar coordinates, is exponentially linearly stable in self-similar coordinates with the natural scaling. This result, which is valid for functions in a weighted L2L^2 space and in the un-weighted L2L^2 space with a mild symmetry condition, answers a question from the monograph by Albritton et al. Moreover, we prove that in physical coordinates the linearization around the power law vortex cannot generate an unstable C0C_0-semigroup.

Keywords

Cite

@article{arxiv.2411.13397,
  title  = {Stability of the Inviscid Power-Law Vortex},
  author = {Tim Binz and Matei P. Coiculescu},
  journal= {arXiv preprint arXiv:2411.13397},
  year   = {2026}
}

Comments

The previous version had an error in Lemma 6.4. The operator K is not dissipative unless a weighted L^2 space is used. If the space is thus changed, we can obtain stability without symmetry conditions. The result for the unweighted L^2 required a mild symmetry condition. The proof is otherwise unchanged. 34 pages