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<article article-type="research-article" dtd-version="1.3" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xml:lang="ru"><front><journal-meta><journal-id journal-id-type="publisher-id">dan</journal-id><journal-title-group><journal-title xml:lang="ru">Доклады Национальной академии наук Беларуси</journal-title><trans-title-group xml:lang="en"><trans-title>Doklady of the National Academy of Sciences of Belarus</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">1561-8323</issn><issn pub-type="epub">2524-2431</issn><publisher><publisher-name>The Republican Unitary Enterprise Publishing House "Belaruskaya Navuka"</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.29235/1561-8323-2020-64-6-747-756</article-id><article-id custom-type="elpub" pub-id-type="custom">dan-936</article-id><article-categories><subj-group subj-group-type="heading"><subject>Research Article</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="ru"><subject>ТЕХНИЧЕСКИЕ НАУКИ</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>TECHNICAL SCIENCES</subject></subj-group></article-categories><title-group><article-title>Особенности самовоспламенения паров н-декана в воздухе при температурах 600–800 К</article-title><trans-title-group xml:lang="en"><trans-title>Specific features of n-decane vapors self-ignition in air at temperatures of 600–800 K</trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Лещевич</surname><given-names>В. В.</given-names></name><name name-style="western" xml:lang="en"><surname>Leschevich</surname><given-names>V. V.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Лещевич Владимир Владимирович – канд. физ.-мат. наук, ст. науч. сотрудник</p><p>ул. П. Бровки, 15, 220072, Минск</p></bio><bio xml:lang="en"><p>Leschevich Vladimir V. – Ph. D. (Physics and Mathematics), Senior researcher</p><p>15, P. Brovka Str., 220072, Minsk</p></bio><email xlink:type="simple">v.leschevich@dnp.itmo.by</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Пенязьков</surname><given-names>О. Г.</given-names></name><name name-style="western" xml:lang="en"><surname>Penyazkov</surname><given-names>O. G.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Пенязьков Олег Глебович – академик, д-р физ.-мат. наук, директор</p><p>ул. П. Бровки, 15, 220072, Минск</p></bio><bio xml:lang="en"><p>Penyazkov Oleg G. – Academician, D. Sc. (Physics and Mathematics), Director</p><p>15, P. Brovka Str., 220072, Minsk</p></bio><email xlink:type="simple">penyaz@dnp.itmo.by</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Шимченко</surname><given-names>С. Ю.</given-names></name><name name-style="western" xml:lang="en"><surname>Shimchenko</surname><given-names>S. Yu.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Шимченко Сергей Юрьевич – науч. сотрудник</p><p>ул. П. Бровки, 15, 220072, Минск</p></bio><bio xml:lang="en"><p>Shimchenko Sergey Yu. – Researcher</p><p>15, P. Brovka Str., 220072, Minsk</p></bio><email xlink:type="simple">sergey.shimchenko@gmail.com</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Институт тепло- и массообмена имени А. В. Лыкова Национальной академии наук Беларуси</institution></aff><aff xml:lang="en"><institution>A. V. Luikov Heat and Mass Transfer Institute of the National Academy of Sciences of Belarus</institution></aff></aff-alternatives><pub-date pub-type="collection"><year>2020</year></pub-date><pub-date pub-type="epub"><day>31</day><month>12</month><year>2020</year></pub-date><volume>64</volume><issue>6</issue><elocation-id>747–756</elocation-id><permissions><copyright-statement>Copyright &amp;#x00A9; Лещевич В.В., Пенязьков О.Г., Шимченко С.Ю., 2020</copyright-statement><copyright-year>2020</copyright-year><copyright-holder xml:lang="ru">Лещевич В.В., Пенязьков О.Г., Шимченко С.Ю.</copyright-holder><copyright-holder xml:lang="en">Leschevich V.V., Penyazkov O.G., Shimchenko S.Y.</copyright-holder><license xml:lang="ru" license-type="creative-commons-attribution" xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:type="simple"><license-p>Данная работа распространяется под лицензией Creative Commons Attribution 4.0.</license-p></license><license xml:lang="en" license-type="creative-commons-attribution" xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:type="simple"><license-p>This work is licensed under a Creative Commons Attribution 4.0 License.</license-p></license></permissions><self-uri xlink:href="https://doklady.belnauka.by/jour/article/view/936">https://doklady.belnauka.by/jour/article/view/936</self-uri><abstract><p>В условиях быстрого адиабатического сжатия изучены особенности самовоспламенения паров н-декана в воздухе при температуре 600–800 К, давлении 0,8–1,2 МПа, эквивалентных отношениях ϕ = 0,5–1,5 и постоянной плотности смеси 5,0 ± 0,5 кг/м3 . Установлены температурно-концентрационные пределы перехода от одностадийного к двухстадийному режиму самовоспламенения. Многоракурсная съемка обнаружила, что в зависимости от температуры «горячая» стадия процесса всегда возникает и развивается вблизи поверхности поршня либо торцевой стенки цилиндра сжатия, сопровождается одновременным переносом образованных очагов внутрь камеры сгорания, после чего происходит близкое к однородному самовоспламенение оставшейся смеси. Фотографии холодного пламени паров н-декана позволили определить пространственное положение очага самовоспламенения первой стадии – вблизи поверхности поршня. Установлено, что вблизи поверхности поршня на оси камеры находится застойная зона, вызванная вихревым тороидальным течением газа, в которой химическая реакция возникает с запозданием. Показано, что по мере увеличения парциального давления паров н-декана при сжатии процесс неравновесной конденсации топлива вблизи стенок камеры сгорания приводит к существенному перераспределению концентрации и температуры смеси по объему, что предопределяет локальные особенности ее последующего самовоспламенения</p></abstract><trans-abstract xml:lang="en"><p>Experiments of n-decane/air self-ignition at the temperature range 600–800 K were carried out by rapid compression machine. It allowed obtaining temperature-concentration limits of transition from single-stage to two-stage ignition. High-speed video recording has let established that hot stage ignition always initiates near the piston surface or quartz window. These locations depend on gas temperature. Combustion of the test mixture occurs in the entire volume after that. Couple sequential photos of cool flame shows that it starts same near piston surface and has a complicated volumetric structure caused by the roll-up gas vortex. It is shown that partial n-decane pressure increasing during compression causes the non-equilibrium condensation process near the inner surfaces of combustion chamber. This leads to significant redistribution of n-decane concentration and determines local characteristics self-ignition of n-decane/air mixture.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>двухстадийное самовоспламенение</kwd><kwd>н-декан</kwd><kwd>установка быстрого сжатия</kwd><kwd>холодное пламя</kwd><kwd>конденсация</kwd><kwd>отрицательный температурный коэффициент</kwd></kwd-group><kwd-group xml:lang="en"><kwd>two-stage ignition</kwd><kwd>n-decane</kwd><kwd>rapid compression machine</kwd><kwd>cool flame</kwd><kwd>condensation</kwd><kwd>negative temperature coefficient</kwd></kwd-group></article-meta></front><back><ref-list><title>References</title><ref id="cit1"><label>1</label><citation-alternatives><mixed-citation xml:lang="ru">Experimental formulation and kinetic model for JP-8 surrogate mixtures / Α. 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