{ "id": "1008.1546", "version": "v2", "published": "2010-08-09T17:07:00.000Z", "updated": "2011-11-01T01:42:26.000Z", "title": "Kolmogorov's Theory of Turbulence and Inviscid Limit of the Navier-Stokes Equations in $\\R^3$", "authors": [ "Gui-Qiang G. Chen", "James Glimm" ], "categories": [ "math.AP", "math-ph", "math.MP" ], "abstract": "We are concerned with the inviscid limit of the Navier-Stokes equations to the Euler equations in $\\R^3$. We first observe that a pathwise Kolmogorov hypothesis implies the uniform boundedness of the $\\alpha^{th}$-order fractional derivative of the velocity for some $\\alpha>0$ in the space variables in $L^2$, which is independent of the viscosity $\\mu>0$. Then it is shown that this key observation yields the $L^2$-equicontinuity in the time and the uniform bound in $L^q$, for some $q>2$, of the velocity independent of $\\mu>0$. These results lead to the strong convergence of solutions of the Navier-Stokes equations to a solution of the Euler equations in $\\R^3$. We also consider passive scalars coupled to the incompressible Navier-Stokes equations and, in this case, find the weak-star convergence for the passive scalars with a limit in the form of a Young measure (pdf depending on space and time). Not only do we offer a framework for mathematical existence theories, but also we offer a framework for the interpretation of numerical solutions through the identification of a function space in which convergence should take place, with the bounds that are independent of $\\mu>0$, that is in the high Reynolds number limit.", "revisions": [ { "version": "v2", "updated": "2011-11-01T01:42:26.000Z" } ], "analyses": { "keywords": [ "navier-stokes equations", "inviscid limit", "kolmogorovs theory", "euler equations", "turbulence" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2010arXiv1008.1546C" } } }