<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>Equivalence of low frequency stability conditions for multidimensional detonations in three models of combustion</dc:title>
<dc:creator>Helge Jenssen</dc:creator><dc:creator>Gregory Lyng</dc:creator><dc:creator>Mark Williams</dc:creator>
<dc:subject>76L05</dc:subject><dc:subject>35B35</dc:subject><dc:subject>multidimensional detonations</dc:subject><dc:subject>stability</dc:subject><dc:subject>Evans function</dc:subject>
<dc:description>We use the classical normal mode approach of hydrodynamic stability theory to define stability determinants (Evans functions) for multidimensional strong detonations in three commonly studied models of combustion: the full reactive Navier-Stokes ($\RNS$) model, and the simpler Zeldovich-von Neumann-D\&quot;oring ($\ZND$) and Chapman-Jouguet (CJ) models. The determinants are functions of frequencies $(\lambda,\eta)$, where $\lambda$ is a complex variable dual to the time variable, and $\eta\in\bR^{d-1}$ is dual to the transverse spatial variables. The zeros of these determinants in $\Re\lambda&gt;0$ correspond to perturbations that grow exponentially with time.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2005</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2005.54.2685</dc:identifier>
<dc:source>10.1512/iumj.2005.54.2685</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 54 (2005) 1 - 64</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>