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On approximate solutions of semilinear evolution equations II. Generalizations, and applications to Navier-Stokes equations

2007/09/30 by Carlo Morosi, Livio Pizzocchero · 6 citations
Mathematics · Physics and Astronomy · #math.AP #math-ph #math.MP #msc:35A35 #msc:35Q30 #msc:65M60

paper · pdf · doi:10.1142/s0129055x08003407

published as Rev. Math. Phys. 20(6) (2008), 625-706 · LaTeX, 84 pages. The final version published in Reviews in Mathematical Physics

arxiv created 2008/07/17 · arxiv updated 2009/12/01

Abstract

In our previous paper [12] (Rev. Math. Phys. 16, 383-420 (2004)), a general framework was outlined to treat the approximate solutions of semilinear evolution equations; more precisely, a scheme was presented to infer from an approximate solution the existence (local or global in time) of an exact solution, and to estimate their distance. In the first half of the present work the abstract framework of \citeuno is extended, so as to be applicable to evolutionary PDEs whose nonlinearities contain derivatives in the space variables. In the second half of the paper this extended framework is applied to theincompressible Navier-Stokes equations, on a torus Td of any dimension. In this way a number of results are obtained in the setting of the Sobolev spaces Hn(Td), choosing the approximate solutions in a number of different ways. With the simplest choices we recover local existence of the exact solution for arbitrary data and external forces, as well as global existence for small data and forces. With the supplementary assumption of exponential decay in time for the forces, the same decay law is derived for the exact solution with small (zero mean) data and forces. The interval of existence for arbitrary data, the upper bounds on data and forces for global existence, and all estimates on the exponential decay of the exact solution are derived in a fully quantitative way (i.e., giving the values of all the necessary constants; this makes a difference with most of the previous literature). Nextly, the Galerkin approximate solutions are considered and precise, still quantitative estimates are derived for their Hn distance from the exact solution; these are global in time for small data and forces (with exponential time decay of the above distance, if the forces decay similarly).

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