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<top_article>
<mrnumber>MR2730622</mrnumber>
<author>R. FARWIG, H. KOZONO and H. SOHR</author>
<author_utf8>R. FARWIG, H. KOZONO and H. SOHR</author_utf8>
<title>Global Weak Solutions of the Navier-Stokes System with Nonzero Boundary Conditions</title>
<journal>Funkcialaj Ekvacioj. Serio Internacia</journal>
<volume>53</volume>
<year>2010</year>
<page>231--247</page>
<url_pdf>http://fe.math.kobe-u.ac.jp/FE/FullPapers/53-2/53_231.pdf</url_pdf>
<mathsci_link>http://www.ams.org/mathscinet-getitem?mr=MR2730622</mathsci_link>
<abstract>Consider the Navier-Stokes equations in a smooth bounded domain $\Omega\subset \mathbf{R}^3$ and a time interval $[0,T)$, $0&#60;T\leq\infty$. It is well-known that there exists at least one global weak solution $u$ with vanishing boundary values $u|_{\partial\Omega}=0$ for any given initial value $u_0\in L_\sigma^2(\Omega)$, external force $f=\div F$, $F\in L^2(0,T;L^2(\Omega))$, and satisfying the strong energy inequality. Our aim is to extend this existence result to a much larger class of global in time &#147;'Leray-Hopf type&#148; weak solutions $u$ with nonzero boundary values $u|_{\partial\Omega}=g\in W^{1/2,2}(\partial\Omega)$.  As for usual weak solutions we do not need any smallness condition on $g$; indeed, our generalized weak solutions $u$ exist globally in time. The solutions will satisfy an energy estimate with exponentially increasing terms in time, but for simply connected domains the energy increases at most linearly in time.</abstract>
<keywords>Navier-Stokes equations, Weak solution, Nonhomogeneous boundary values, Strong energy inequality.</keywords>
<subject>76D05, 35Q30, 35J65.</subject>
<fesi_info>
  <FILE>53-231</FILE>
  <YEAR>2010</YEAR>
  <TITLE>Global Weak Solutions of the Navier-Stokes System with Nonzero Boundary Conditions</TITLE>
  <AUTHOR>R. FARWIG, H. KOZONO and H. SOHR</AUTHOR>
  <AUTHOR_utf8>R. FARWIG, H. KOZONO and H. SOHR</AUTHOR_utf8>
</fesi_info>

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