<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>Blow-up for a degenerate diffusion problem not in divergence form</dc:title>
<dc:creator>Arturo de Pablo</dc:creator><dc:creator>Raul Ferreira</dc:creator><dc:creator>Julio Rossi</dc:creator>
<dc:subject>35B40</dc:subject><dc:subject>35B35</dc:subject><dc:subject>35K65</dc:subject><dc:subject>blow-up</dc:subject><dc:subject>asymptotic behaviour</dc:subject><dc:subject>nonlinear boundary conditions</dc:subject>
<dc:description>We study the behaviour of solutions of the nonlinear diffusion equation in the half-line, $\mathbb{R}_{+} = (0,\infty)$, with a nonlinear boundary condition, \[ \begin{cases} u_t = uu_{xx}, \quad (x,t) \in \mathbb{R}_{+} \times (0,T),\\ -u_{x}(0,t) = u^{p}(0,t), \quad t \in (0,T),\\ u(x,0) = u_0(x), \quad x \in \mathbb{R}_{+},\\ \end{cases} \] with $p$ greater than $0$. We describe, in terms of $p$ and the initial datum, when the solution is global in time and when it blows up in finite time. For blowing up solutions we find the blow-up rate and the blow-up set and we describe the asymptotic behaviour close to the blow-up time in terms of a self-similar profile. The stationary character of the support is proved both for global solutions and blowing-up solutions. Also we obtain results for the problem in a bounded interval.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2006</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2006.55.2725</dc:identifier>
<dc:source>10.1512/iumj.2006.55.2725</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 55 (2006) 955 - 974</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>