<?xml version="1.0" encoding="UTF-8"?>
<collection xmlns="http://www.loc.gov/MARC21/slim">
 <record>
  <leader>     caa a22        4500</leader>
  <controlfield tag="001">378884174</controlfield>
  <controlfield tag="003">CHVBK</controlfield>
  <controlfield tag="005">20180305123439.0</controlfield>
  <controlfield tag="007">cr unu---uuuuu</controlfield>
  <controlfield tag="008">161128s2004    xx      s     000 0 eng  </controlfield>
  <datafield tag="024" ind1="7" ind2="0">
   <subfield code="a">10.2478/cmam-2004-0007</subfield>
   <subfield code="2">doi</subfield>
  </datafield>
  <datafield tag="035" ind1=" " ind2=" ">
   <subfield code="a">(NATIONALLICENCE)gruyter-10.2478/cmam-2004-0007</subfield>
  </datafield>
  <datafield tag="245" ind1="0" ind2="2">
   <subfield code="a">A Class of Singularly Perturbed Convection-Diffusion Problems with a Moving Interior Layer. An a Posteriori Adaptive Mesh Technique</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
  </datafield>
  <datafield tag="520" ind1="3" ind2=" ">
   <subfield code="a">We study numerical approximations for a class of singularly perturbed convection-diffusion type problems with a moving interior layer. In a domain (segment) with a moving interface between two subdomains, we consider an initial boundary value problem for a singularly perturbed parabolic convection-diffusion equation. Convection ﬂuxes on the subdomains are directed towards the interface. The solution of this problem has a moving transition layer in the neighbourhood of the interface. Unlike problems with a stationary layer, the solution exhibits singular behaviour also with respect to the time variable. Well-known upwind ﬁnite difference schemes for such problems do not converge ε-uniformly in the uniform norm. In the case of rectangular meshes which are (a priori or a posteriori ) locally condensed in the transition layer. However, the condition for convergence can be considerably weakened if we take the geometry of the layer into account, i.e., if we introduce a new coordinate system which captures the interface. For the problem in such a coordinate system, one can use either an a priori, or an a posteriori adaptive mesh technique. Here we construct a scheme on a posteriori adaptive meshes (based on the solution gradient), whose solution converges ‘almost ε-uniformly'.</subfield>
  </datafield>
  <datafield tag="540" ind1=" " ind2=" ">
   <subfield code="a">This article is distributed under the terms of the Creative Commons Attribution Non-Commercial License, which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">singular perturbation problem</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">convection-diffusion equation</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">moving interior/transition layer</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">a posteriori adaptive mesh</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">almost ε-uniform convergence</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Shishkin</subfield>
   <subfield code="D">Grigory I.</subfield>
   <subfield code="u">Institute of Mathematics and Mechanics, Ural Branch of Russian Academy of Science, 16 S. Kovalevskaya St., 620219 Ekaterinburg, Russia</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Shishkina</subfield>
   <subfield code="D">Lidia P.</subfield>
   <subfield code="u">Institute of Mathematics and Mechanics, Ural Branch of Russian Academy of Science, 16 S. Kovalevskaya St., 620219 Ekaterinburg, Russia</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Hemker</subfield>
   <subfield code="D">Pieter W.</subfield>
   <subfield code="u">CWI, P.O. Box 94079, 1090 GB Amsterdam, The Netherlands</subfield>
  </datafield>
  <datafield tag="773" ind1="0" ind2=" ">
   <subfield code="t">Computational Methods in Applied Mathematics</subfield>
   <subfield code="d">De Gruyter</subfield>
   <subfield code="g">4/1(2004), 105-127</subfield>
   <subfield code="x">1609-4840</subfield>
   <subfield code="q">4:1&lt;105</subfield>
   <subfield code="1">2004</subfield>
   <subfield code="2">4</subfield>
   <subfield code="o">cmam</subfield>
  </datafield>
  <datafield tag="856" ind1="4" ind2="0">
   <subfield code="u">https://doi.org/10.2478/cmam-2004-0007</subfield>
   <subfield code="q">text/html</subfield>
   <subfield code="z">Onlinezugriff via DOI</subfield>
  </datafield>
  <datafield tag="908" ind1=" " ind2=" ">
   <subfield code="D">1</subfield>
   <subfield code="a">research article</subfield>
   <subfield code="2">jats</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">856</subfield>
   <subfield code="E">40</subfield>
   <subfield code="u">https://doi.org/10.2478/cmam-2004-0007</subfield>
   <subfield code="q">text/html</subfield>
   <subfield code="z">Onlinezugriff via DOI</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Shishkin</subfield>
   <subfield code="D">Grigory I.</subfield>
   <subfield code="u">Institute of Mathematics and Mechanics, Ural Branch of Russian Academy of Science, 16 S. Kovalevskaya St., 620219 Ekaterinburg, Russia</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Shishkina</subfield>
   <subfield code="D">Lidia P.</subfield>
   <subfield code="u">Institute of Mathematics and Mechanics, Ural Branch of Russian Academy of Science, 16 S. Kovalevskaya St., 620219 Ekaterinburg, Russia</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Hemker</subfield>
   <subfield code="D">Pieter W.</subfield>
   <subfield code="u">CWI, P.O. Box 94079, 1090 GB Amsterdam, The Netherlands</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">773</subfield>
   <subfield code="E">0-</subfield>
   <subfield code="t">Computational Methods in Applied Mathematics</subfield>
   <subfield code="d">De Gruyter</subfield>
   <subfield code="g">4/1(2004), 105-127</subfield>
   <subfield code="x">1609-4840</subfield>
   <subfield code="q">4:1&lt;105</subfield>
   <subfield code="1">2004</subfield>
   <subfield code="2">4</subfield>
   <subfield code="o">cmam</subfield>
  </datafield>
  <datafield tag="900" ind1=" " ind2="7">
   <subfield code="b">CC0</subfield>
   <subfield code="u">http://creativecommons.org/publicdomain/zero/1.0</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="898" ind1=" " ind2=" ">
   <subfield code="a">BK010053</subfield>
   <subfield code="b">XK010053</subfield>
   <subfield code="c">XK010000</subfield>
  </datafield>
  <datafield tag="949" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="F">NATIONALLICENCE</subfield>
   <subfield code="b">NL-gruyter</subfield>
  </datafield>
 </record>
</collection>
