On the vanishing viscosity limit in a disk

dc.creatorKelliher, James P
dc.date2006-12-10
dc.date.accessioned2026-07-07T12:53:14Z
dc.date.available2026-07-07T12:53:14Z
dc.descriptionWe say that the solution u to the Navier-Stokes equations converges to a solution v to the Euler equations in the vanishing viscosity limit if u converges to v in the energy norm uniformly over a finite time interval. Working specifically in the unit disk, we show that a necessary and sufficient condition for the vanishing viscosity limit to hold is the vanishing with the viscosity of the time-space average of the energy of u in a boundary layer of width proportional to the viscosity due to modes (eigenfunctions of the Stokes operator) whose frequencies in the radial or the tangential direction lie between L and M. Here, L must be of order less than 1/(viscosity) and M must be of order greater than 1/(viscosity).
dc.identifierhttps://arxiv.org/abs/math-ph/0612027
dc.identifierhttp://arxiv.org/abs/math-ph/0612027
dc.identifierMathematische Annalen, 343:701-726, 2009
dc.identifierdoi:10.1007/s00208-008-0287-3
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/223556
dc.subjectMathematical Physics
dc.subject76D05; 76B99; 76D99
dc.titleOn the vanishing viscosity limit in a disk
dc.typetext

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