The vanishing viscosity limit for incompressible fluids in two dimensions

dc.contributor.advisorVishik, Mikhailen
dc.creatorKelliher, James Patricken
dc.date.accessioned2008-08-28T22:07:42Zen
dc.date.available2008-08-28T22:07:42Zen
dc.date.issued2005en
dc.descriptiontexten
dc.description.abstractThe Navier-Stokes equations describe the motion of an incompressible fluid of constant density and constant positive viscosity. With zero viscosity, the Navier-Stokes equations become the Euler equations. A question of longstanding interest to mathematicians and physicists is whether, as the viscosity goes to zero, a solution to the Navier-Stokes equations converges, in an appropriate sense, to a solution to the Euler equations: the so-called “vanishing viscosity” or “inviscid” limit. We investigate this question in three settings: in the whole plane, in a bounded domain in the plane, and for radially symmetric solutions in the whole plane. Working in the whole plane and in a bounded domain, we assume a particular bound on the growth of the L p -norms of the initial vorticity (curl of the velocity) with p, and obtain a bound on the convergence rate in the vanishing viscosity limit. This is the same class of initial vorticities considered by Yudovich and shown to imply uniqueness of the solution to the Euler equations in a bounded domain lying in Euclidean space of dimension 2 or greater. For radially symmetric initial vorticities we obtain a more precise bound on the convergence rate as a function of the smoothness of its initial vorticity as measured by its norm in a Sobolev space or in certain Besov spaces. We also consider the questions of existence, uniqueness, and regularity of solutions to the Navier-Stokes and Euler equations, as necessary, to make sense of the vanishing viscosity limit. In particular, we investigate properties of the flow for solutions to the Euler equations in the whole plane. We construct a specific example of an initial vorticity for which there exists a unique solution to the Euler equations whose associated flow lies in no H¨older space of positive exponent for any positive time. This example is an adaptation of a bounded-vorticity example of Bahouri and Chemin’s, which they show has a flow lying in no H¨older space of exponent greater than an exponentially decreasing function of time.
dc.description.departmentMathematicsen
dc.format.mediumelectronicen
dc.identifierb59923350en
dc.identifier.oclc61387329en
dc.identifier.proqst3174486en
dc.identifier.urihttp://hdl.handle.net/2152/1589en
dc.language.isoengen
dc.rightsCopyright is held by the author. Presentation of this material on the Libraries' web site by University Libraries, The University of Texas at Austin was made possible under a limited license grant from the author who has retained all copyrights in the works.en
dc.subject.lcshNavier-Stokes equationsen
dc.subject.lcshFluid dynamics--Mathematicsen
dc.subject.lcshViscous flow--Mathematicsen
dc.titleThe vanishing viscosity limit for incompressible fluids in two dimensionsen
dc.type.genreThesisen
thesis.degree.departmentMathematicsen
thesis.degree.disciplineMathematicsen
thesis.degree.grantorThe University of Texas at Austinen
thesis.degree.levelDoctoralen
thesis.degree.nameDoctor of Philosophyen

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