Onsager's conjecture and anomalous dissipation on domains with boundary
arXiv:1803.05416 · doi:10.1137/18M1178864
Abstract
We give a localized regularity condition for energy conservation of weak solutions of the Euler equations on a domain , , with boundary. In the bulk of fluid, we assume Besov regularity of the velocity . On an arbitrary thin neighborhood of the boundary, we assume boundedness of velocity and pressure and, at the boundary, we assume continuity of wall-normal velocity. We also prove two theorems which establish that the global viscous dissipation vanishes in the inviscid limit for Leray--Hopf solutions of the Navier-Stokes equations under the similar assumptions, but holding uniformly in a thin boundary layer of width when in the interior for any . The first theorem assumes continuity of the velocity in the boundary layer whereas the second assumes a condition on the vanishing of energy dissipation within the layer. In both cases, strong convergence holds to a weak solution of the Euler equations. Finally, if a strong Euler solution exists in the background, we show that equicontinuity at the boundary within a strip alone suffices to conclude the absence of anomalous dissipation.
23 pages, 1 figure. Theorem 3 added in version 2. Sharpened the interior regularity assumption on the velocity in Theorems 1,2 and 3 in version 3
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Cited by in corpus (15)
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