<oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:title>Concentration-diffusion effects in viscous incompressible flows</dc:title>
<dc:creator>Lorenzo Brandolese</dc:creator>
<dc:subject>76D05</dc:subject><dc:subject>35Q30</dc:subject><dc:subject>Navier-Stokes</dc:subject><dc:subject>asymptotic profiles</dc:subject><dc:subject>asymptotic behavior</dc:subject><dc:subject>far-field</dc:subject><dc:subject>flow map</dc:subject><dc:subject>analyticity</dc:subject><dc:subject>symmetry</dc:subject><dc:subject>spatial spreading</dc:subject><dc:subject>lower bound</dc:subject><dc:subject>pointwise estimates</dc:subject><dc:subject>decay rate</dc:subject><dc:subject>singularities</dc:subject>
<dc:description>Given a finite sequence of times $0 &lt; t_{1} &lt; \dots &lt; t_{N}$, we construct an example of a smooth solution of the free nonstationnary Navier-Stokes equations in $\mathbb{R}^d$, $d = 2,3$, such that: (i) The velocity field $u(x,t)$ is spatially poorly localized at the beginning of the evolution but tends to concentrate until, as the time $t$ approaches $t_{1}$, it becomes well localized. (ii) Then $u$ spreads out again after $t_{1}$, and such concentration-diffusion phenomena are later reproduced near the instants $t_{2}$, $t_{3}$, \dots .</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2009</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2009.58.3504</dc:identifier>
<dc:source>10.1512/iumj.2009.58.3504</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 58 (2009) 789 - 806</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>