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      Reflections on Dubinskii's nonlinear compact embedding theorem

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          Abstract

          We present an overview of a result by Ju. A. Dubinskii [Mat. Sb. 67 (109) (1965); translated in Amer. Math. Soc. Transl. (2) 67 (1968)], concerning the compact embedding of a seminormed set in \(L^p(0,T; \mathcal{A}_0)\), where \(\mathcal{A}_0\) is a Banach space and \(p \in [1,\infty]\); we establish a variant of Dubinskii's theorem, where a seminormed nonnegative cone is used instead of a seminormed set; and we explore the connections of these results with a nonlinear compact embedding theorem due to E. Maitre [Int. J. Math. Math. Sci. 27 (2003)].

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          Existence and equilibration of global weak solutions to finitely extensible nonlinear bead-spring chain models for dilute polymers

          We show the existence of global-in-time weak solutions to a general class of coupled FENE-type bead-spring chain models that arise from the kinetic theory of dilute solutions of polymeric liquids with noninteracting polymer chains. The class of models involves the unsteady incompressible Navier-Stokes equations in a bounded domain in two or three space dimensions for the velocity and the pressure of the fluid, with an elastic extra-stress tensor appearing on the right-hand side in the momentum equation. The extra-stress tensor stems from the random movement of the polymer chains and is defined by the Kramers expression through the associated probability density function that satisfies a Fokker-Planck-type parabolic equation, a crucial feature of which is the presence of a center-of-mass diffusion term. We require no structural assumptions on the drag term in the Fokker-Planck equation; in particular, the drag term need not be corotational. With a square-integrable and divergence-free initial velocity datum for the Navier-Stokes equation and a nonnegative initial probability density function for the Fokker-Planck equation, which has finite relative entropy with respect to the Maxwellian of the model, we prove the existence of a global-in-time weak solution to the coupled Navier-Stokes-Fokker-Planck system. It is also shown that in the absence of a body force, the weak solution decays exponentially in time to the equilibrium solution, at a rate that is independent of the choice of the initial datum and of the centre-of-mass diffusion coefficient.
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            Author and article information

            Journal
            10 January 2011
            2011-04-16
            Article
            10.2298/PIM1205095B
            1101.1990
            e602ea9f-255a-4118-8735-d18f4554f4c6

            http://arxiv.org/licenses/nonexclusive-distrib/1.0/

            History
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            Publ. Inst. Math. (Belgrade) (N.S.) 91(105) (2012), 95-110
            17 pages, 1 figure
            math.AP math.FA

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