{ "id": "1412.6587", "version": "v1", "published": "2014-12-20T03:12:19.000Z", "updated": "2014-12-20T03:12:19.000Z", "title": "Approximation of 2D Euler Equations by the Second-Grade Fluid Equations with Dirichlet Boundary Conditions", "authors": [ "Milton C. Lopes Filho", "Helena J. Nussenzveig Lopes", "Edriss S. Titi", "Aibin Zang" ], "comment": "20pages,1figure", "categories": [ "math.AP" ], "abstract": "The second-grade fluid equations are a model for viscoelastic fluids, with two parameters: $\\alpha > 0$, corresponding to the elastic response, and $\\nu > 0$, corresponding to viscosity. Formally setting these parameters to $0$ reduces the equations to the incompressible Euler equations of ideal fluid flow. In this article we study the limits $\\alpha, \\nu \\to 0$ of solutions of the second-grade fluid system, in a smooth, bounded, two-dimensional domain with no-slip boundary conditions. This class of problems interpolates between the Euler-$\\alpha$ model ($\\nu = 0$), for which the authors recently proved convergence to the solution of the incompressible Euler equations, and the Navier-Stokes case ($\\alpha = 0$), for which the vanishing viscosity limit is an important open problem. We prove three results. First, we establish convergence of the solutions of the second-grade model to those of the Euler equations provided $\\nu = \\mathcal{O}(\\alpha^2)$, as $\\alpha \\to 0$, extending the main result in [19]. Second, we prove equivalence between convergence (of the second-grade fluid equations to the Euler equations) and vanishing of the energy dissipation in a suitably thin region near the boundary, in the asymptotic regime $\\nu = \\mathcal{O}(\\alpha^{6/5})$, $\\nu/\\alpha^2 \\to \\infty$ as $\\alpha \\to 0$. This amounts to a convergence criterion similar to the well-known Kato criterion for the vanishing viscosity limit of the Navier-Stokes equations to the Euler equations. Finally, we obtain an extension of Kato's classical criterion to the second-grade fluid model, valid if $\\alpha = \\mathcal{O}(\\nu^{3/2})$, as $\\nu \\to 0$. The proof of all these results relies on energy estimates and boundary correctors, following the original idea by Kato.", "revisions": [ { "version": "v1", "updated": "2014-12-20T03:12:19.000Z" } ], "analyses": { "subjects": [ "35Q30", "76D05", "76D10" ], "keywords": [ "second-grade fluid equations", "dirichlet boundary conditions", "2d euler equations", "vanishing viscosity limit", "incompressible euler equations" ], "publication": { "doi": "10.1007/s00021-015-0207-8", "journal": "Journal of Mathematical Fluid Mechanics", "year": 2015, "month": "Jun", "volume": 17, "number": 2, "pages": 327 }, "note": { "typesetting": "TeX", "pages": 20, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2015JMFM...17..327L" } } }