No anomalous dissipation in two-dimensional incompressible fluids

Fuente: arXiv
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Autori principali: De Rosa, Luigi, Park, Jaemin
Natura: Preprint
Pubblicazione: 2024
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author De Rosa, Luigi
Park, Jaemin
author_facet De Rosa, Luigi
Park, Jaemin
contents We prove that any sequence of vanishing viscosity Leray-Hopf solutions to the periodic two-dimensional incompressible Navier-Stokes equations does not display anomalous dissipation if the initial vorticity is a measure with positive singular part. A key step in the proof is the use of the Delort-Majda concentration-compactness argument to exclude formation of atoms in the vorticity measure, which in particular implies that the limiting velocity is an admissible weak solution to Euler. This is the first result proving absence of dissipation in a class of solutions in which the velocity fails to be strongly compact in $L^2$, putting two-dimensional turbulence in sharp contrast with respect to that in three dimensions. Moreover, our proof reveals that the amount of energy dissipation can be bounded by the vorticity measure of a disk of size $\sqrt ν$, matching the two-dimensional Kolmogorov dissipative length scale which is expected to be sharp.
format Preprint
id arxiv_https___arxiv_org_abs_2403_04668
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle No anomalous dissipation in two-dimensional incompressible fluids
De Rosa, Luigi
Park, Jaemin
Analysis of PDEs
We prove that any sequence of vanishing viscosity Leray-Hopf solutions to the periodic two-dimensional incompressible Navier-Stokes equations does not display anomalous dissipation if the initial vorticity is a measure with positive singular part. A key step in the proof is the use of the Delort-Majda concentration-compactness argument to exclude formation of atoms in the vorticity measure, which in particular implies that the limiting velocity is an admissible weak solution to Euler. This is the first result proving absence of dissipation in a class of solutions in which the velocity fails to be strongly compact in $L^2$, putting two-dimensional turbulence in sharp contrast with respect to that in three dimensions. Moreover, our proof reveals that the amount of energy dissipation can be bounded by the vorticity measure of a disk of size $\sqrt ν$, matching the two-dimensional Kolmogorov dissipative length scale which is expected to be sharp.
title No anomalous dissipation in two-dimensional incompressible fluids
topic Analysis of PDEs
url https://arxiv.org/abs/2403.04668