<?xml version="1.0" encoding="UTF-8"?>
<collection xmlns="http://www.loc.gov/MARC21/slim">
 <record>
  <leader>     caa a22        4500</leader>
  <controlfield tag="001">475810481</controlfield>
  <controlfield tag="003">CHVBK</controlfield>
  <controlfield tag="005">20180406123757.0</controlfield>
  <controlfield tag="007">cr unu---uuuuu</controlfield>
  <controlfield tag="008">170329e20000501xx      s     000 0 eng  </controlfield>
  <datafield tag="024" ind1="7" ind2="0">
   <subfield code="a">10.1007/BF02699378</subfield>
   <subfield code="2">doi</subfield>
  </datafield>
  <datafield tag="035" ind1=" " ind2=" ">
   <subfield code="a">(NATIONALLICENCE)springer-10.1007/BF02699378</subfield>
  </datafield>
  <datafield tag="245" ind1="0" ind2="0">
   <subfield code="a">Conditions of self-ignition upon pulsed high-pressure injection of combustible gases into a bounded space</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[V. Baev, A. Buzukov, V. Shumskii]</subfield>
  </datafield>
  <datafield tag="520" ind1="3" ind2=" ">
   <subfield code="a">The temperature of a fuel-air mixture in the vicinity of a contact discontinuity formed in the process of exhaustion of a combustible gas (hydrogen, methane, and propane) into air after the shock-tube membrane breakdown is quantitatively evaluated. It is shown that conditions necessary for self-ignition of such a mixture are reached only when the shock wave reflected from the tube bottom passes through the mixture. An increase in the initial pressure of air in the tube exerts a dramatic adverse effect on the probability of self-ignition of the mixture. In addition, the calculation shows that favorable conditions for self-ignition of a methane- and propane-air mixtures, even after the secondary compression of the mixture behind the reflected-wave front, are observed only for a comparatively high pressure of the combustible gas prior to its exhaustion into the tube and simultaneously for a low initial pressure of air in the tube. The calculation results are in good agreement with available experimental data for a hydrogen-air mixture.</subfield>
  </datafield>
  <datafield tag="540" ind1=" " ind2=" ">
   <subfield code="a">Kluwer Academic/Plenum Publishers, 2000</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Baev</subfield>
   <subfield code="D">V.</subfield>
   <subfield code="u">Institute of Theoretical and Applied Mechanics, Siberian Division, Russian Academy of Sciences, 630090, Novosibirsk</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Buzukov</subfield>
   <subfield code="D">A.</subfield>
   <subfield code="u">Institute of Theoretical and Applied Mechanics, Siberian Division, Russian Academy of Sciences, 630090, Novosibirsk</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Shumskii</subfield>
   <subfield code="D">V.</subfield>
   <subfield code="u">Institute of Theoretical and Applied Mechanics, Siberian Division, Russian Academy of Sciences, 630090, Novosibirsk</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="773" ind1="0" ind2=" ">
   <subfield code="t">Combustion, Explosion and Shock Waves</subfield>
   <subfield code="d">Springer US</subfield>
   <subfield code="g">36/3(2000-05-01), 283-290</subfield>
   <subfield code="x">0010-5082</subfield>
   <subfield code="q">36:3&lt;283</subfield>
   <subfield code="1">2000</subfield>
   <subfield code="2">36</subfield>
   <subfield code="o">10573</subfield>
  </datafield>
  <datafield tag="856" ind1="4" ind2="0">
   <subfield code="u">https://doi.org/10.1007/BF02699378</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/10.1007/BF02699378</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">Baev</subfield>
   <subfield code="D">V.</subfield>
   <subfield code="u">Institute of Theoretical and Applied Mechanics, Siberian Division, Russian Academy of Sciences, 630090, Novosibirsk</subfield>
   <subfield code="4">aut</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">Buzukov</subfield>
   <subfield code="D">A.</subfield>
   <subfield code="u">Institute of Theoretical and Applied Mechanics, Siberian Division, Russian Academy of Sciences, 630090, Novosibirsk</subfield>
   <subfield code="4">aut</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">Shumskii</subfield>
   <subfield code="D">V.</subfield>
   <subfield code="u">Institute of Theoretical and Applied Mechanics, Siberian Division, Russian Academy of Sciences, 630090, Novosibirsk</subfield>
   <subfield code="4">aut</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">Combustion, Explosion and Shock Waves</subfield>
   <subfield code="d">Springer US</subfield>
   <subfield code="g">36/3(2000-05-01), 283-290</subfield>
   <subfield code="x">0010-5082</subfield>
   <subfield code="q">36:3&lt;283</subfield>
   <subfield code="1">2000</subfield>
   <subfield code="2">36</subfield>
   <subfield code="o">10573</subfield>
  </datafield>
  <datafield tag="900" ind1=" " ind2="7">
   <subfield code="a">Metadata rights reserved</subfield>
   <subfield code="b">Springer special CC-BY-NC licence</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-springer</subfield>
  </datafield>
 </record>
</collection>
