<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>Heteroclinic orbits with fast transitions: a new construction of detonation profiles</dc:title>
<dc:creator>Mark Williams</dc:creator>
<dc:subject>37C29</dc:subject><dc:subject>34E15</dc:subject><dc:subject>80A25</dc:subject><dc:subject>heteroclinic orbits</dc:subject><dc:subject>detonation profiles</dc:subject><dc:subject>ZND equations</dc:subject><dc:subject>reactive Navier-Stokes equations</dc:subject>
<dc:description>We give a direct and elementary construction of strong detonation profiles for the reactive Navier-Stokes equations (RNS), starting with an inviscid template given by a solution to the Zeldovitch-von Neumann-Doering (ZND) equations. Assuming that the viscosity, heat conductivity, and species diffusion coefficients in RNS are all proportional to $\epsilon$, we construct detonation profiles $w^{\epsilon}(x)$ that are exact solutions of RNS which converge in an appropriate sense to the given ZND profile as $\epsilon \to 0$. The construction is explicit in the sense that it produces an arbitrarily high order expansion in powers of $\epsilon$ for $w^{\epsilon}$, and the coefficients in the expansion satisfy simple, explicit ODEs, which are \emph{linear} except in the case of the leading term. Moreover, the leading &quot;slow&quot; term in the expansion is the original ZND profile, and the burned and unburned endstates of each RNS profile $w^{\epsilon}$ coincide with those of the given ZND profile.\par  The method used here is applicable to a variety of singular perturbation problems in which one seeks to construct smooth ``viscous profiles&#39;, involving both slow and fast transition regions, that converge to discontinuous &quot;inviscid profiles&quot; as a viscosity parameter $\epsilon$ tends to $0$. The method is applicable, for example, to second-order systems that cannot be written in conservative form, and can be used to construct solutions with fast transitions in situations, like two-point boundary problems, where no rest points or higher dimensional invariant manifolds are present in the &quot;reduced problem&quot;.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2010</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2010.59.3992</dc:identifier>
<dc:source>10.1512/iumj.2010.59.3992</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 59 (2010) 1145 - 1210</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>