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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">firesmi</journal-id><journal-title-group><journal-title xml:lang="ru">Пожаровзрывобезопасность/Fire and Explosion Safety</journal-title><trans-title-group xml:lang="en"><trans-title>Pozharovzryvobezopasnost/Fire and Explosion Safety</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">0869-7493</issn><issn pub-type="epub">2587-6201</issn><publisher><publisher-name>ФГБОУ ВО «Национальный исследовательский Московский государственный строительный университет»</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.22227/0869-7493.2024.33.02.23-31</article-id><article-id custom-type="elpub" pub-id-type="custom">firesmi-1350</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>ПРОЦЕССЫ ГОРЕНИЯ, ДЕТОНАЦИИ И ВЗРЫВА</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>COMBUSTION, DETONATION AND EXPLOSION PROCESSES</subject></subj-group></article-categories><title-group><article-title>Особенности взрыва антрацита в 20-л камере</article-title><trans-title-group xml:lang="en"><trans-title>Anthracite dust explosion specificities in 20 L chamber</trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0003-2586-8597</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Полетаев</surname><given-names>Н. Л.</given-names></name><name name-style="western" xml:lang="en"><surname>Poletaev</surname><given-names>N. L.</given-names></name></name-alternatives><bio xml:lang="ru"><p>ПОЛЕТАЕВ Николай Львович, д-р техн. наук, ведущий научный сотрудник</p><p>143903, Московская обл., г. Балашиха, мкр. ВНИИПО, 12</p><p>РИНЦ AuthorID: 1093620</p></bio><bio xml:lang="en"><p>Nikolay L. POLETAEV, Dr. Sci. (Eng.), Leading Researcher</p><p>VNIIPO, 12, Balashikha, Moscow Region, 143903</p><p>RISC AuthorID: 1093620</p></bio><email xlink:type="simple">nlpvniipo@mail.ru</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0001-9000-7115</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Сазонов</surname><given-names>М. С.</given-names></name><name name-style="western" xml:lang="en"><surname>Sazonov</surname><given-names>M. S.</given-names></name></name-alternatives><bio xml:lang="ru"><p>САЗОНОВ Михаил Сергеевич, канд. техн. наук, старший научный сотрудник</p><p>650002, Кемеровская обл., Кузбасс, Кемеровский г.о.;г. Кемерово, ул. Институтская, 3, помещ. 1</p><p>РИНЦ AuthorID: 543411</p></bio><bio xml:lang="en"><p>Mikhail S. SAZONOV, Cand. Sci. (Eng.), Senior Researcher</p><p>Institutskaya, 3, room 1, Kemerovo, Kemerovo Region, Kuzbass, 650002</p><p>RISC AuthorID: 543411</p></bio><email xlink:type="simple">m.sazonov@nc-vostnii.ru</email><xref ref-type="aff" rid="aff-2"/></contrib><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0009-0004-3812-9747</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Коптев</surname><given-names>М. Ю.</given-names></name><name name-style="western" xml:lang="en"><surname>Koptev</surname><given-names>M. Yu.</given-names></name></name-alternatives><bio xml:lang="ru"><p>КОПТЕВ Михаил Юрьевич, и.о. заведующего лабораторией борьбы с пылью и пылевзрывозащиты</p><p>650002, Кемеровская обл., Кемеровский г.о.; г. Кемерово, ул. Институтская, 3, помещ. 1</p><p>РИНЦ AuthorID: 893607</p></bio><bio xml:lang="en"><p>Mikhail Yu. KOPTEV, Senior Researcher</p><p>Institutskaya, 3, room 1, Kemerovo, Kemerovo Region, Kuzbass, 650002</p><p>RISC AuthorID:  893607</p></bio><email xlink:type="simple">m.koptev@nc-vostnii.ru</email><xref ref-type="aff" rid="aff-2"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Всероссийский ордена «Знак Почета» научно-исследовательский институт противопожарной обороны Министерства Российской Федерации по делам гражданской обороны, чрезвычайным ситуациям и ликвидации последствий стихийных бедствий</institution><country>Россия</country></aff><aff xml:lang="en"><institution>All-Russian Research Institute for Fire Protection of Ministry of Russian Federation for Civil Defense, Emergencies and Elimination of Consequences of Natural Disasters</institution><country>Russian Federation</country></aff></aff-alternatives><aff-alternatives id="aff-2"><aff xml:lang="ru"><institution>Акционерное общество «Научный центр ВостНИИ по промышленной и экологической безопасности в горной отрасли»</institution><country>Россия</country></aff><aff xml:lang="en"><institution>Joint-Stock Company “Scientific Center of VOSTNII on Industrial and Environmental Safety in the Mining Industry”</institution><country>Russian Federation</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2024</year></pub-date><pub-date pub-type="epub"><day>27</day><month>04</month><year>2024</year></pub-date><volume>33</volume><issue>2</issue><fpage>23</fpage><lpage>31</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Полетаев Н.Л., Сазонов М.С., Коптев М.Ю., 2024</copyright-statement><copyright-year>2024</copyright-year><copyright-holder xml:lang="ru">Полетаев Н.Л., Сазонов М.С., Коптев М.Ю.</copyright-holder><copyright-holder xml:lang="en">Poletaev N.L., Sazonov M.S., Koptev M.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://www.fire-smi.ru/jour/article/view/1350">https://www.fire-smi.ru/jour/article/view/1350</self-uri><abstract><sec><title>Введение</title><p>Введение. Хорошо известен эффект «overdrive», когда аэровзвесь, проявившая взрывоопасность при тестировании в 20-л камере, оказывается безопасной по результатам более надежного тестирования в 1 м3 камере. Завышение взрывоопасности пыли в 20-л камере объясняют предварительным нагревом свежей аэровзвеси пламенем энергоемкого (Eig) источника зажигания. О возможности «overdrive» судят по такому признаку: при Eig = 10 кДж индекс взрыва Kst &lt; 4,5 МПа∙м/с (Proust et al., 2007). Данная статья посвящена выявлению дополнительных признаков «overdrive» в 20-л камере на примере взрывобезопасного антрацита для снижения вероятности упомянутой выше качественной ошибки.</p></sec><sec><title>Анализ публикаций</title><p>Анализ публикаций. Замечен случайный характер проявления взрывоопасности антрацита в широком диапазоне концентраций пыли при Eig = 5 кДж (Cashdollar, Chatrathi, 1993). Наблюдаются две точки перегиба на восходящей ветви зависимости давления взрыва антрацита P от времени t, отвечающие сначала минимуму, а затем максимуму dP/dt соответственно. Все эти особенности могут являться признаками «overdrive» после экспериментальной проверки.</p><p>Антрацит и метод его исследования. Антрацит с содержанием летучих 2,7 % масс. исследован в 20-л камере Сивека, Eig = 10 кДж, с видеосъемкой излучения через смотровое окно.</p></sec><sec><title>Результаты</title><p>Результаты. Получены зависимости интенсивности излучения среды и давления в камере от времени в диапазоне концентраций пыли от 125 до 750 г/м3.</p></sec><sec><title>Обсуждение и выводы</title><p>Обсуждение и выводы. Подтверждены экспериментально и предложены три дополнительных признака эффекта «overdrive» для антрацита: вероятностный характер проявления взрывоопасности; две точки перегиба на восходящей ветви графика P(t); заметное ослабление излучения среды после выгорания источника зажигания и до момента достижения нижней точки перегиба. Давление взрыва превышало 400 кПа и обусловлено, в основном, выгоранием связанного углерода.</p></sec></abstract><trans-abstract xml:lang="en"><sec><title>Introduction</title><p>Introduction. The “overdrive” effect is well known, when dust/air mixture, explosive during testing in a 20 L chamber, turns out to be safe according to the results of more reliable testing in a 1-m3 chamber. The overestimation of the dust explosion hazard in the 20 L chamber is explained by the preheating of the fresh dust/air mixture with the flame of an energy-intensive (Eig) ignition source. The possibility of “overdrive” is judged by the following basis: at Eig = 10 kJ, the explosion index Kst &lt; 4.5 MPa∙m/s (Proust et al., 2007). This paper is devoted to the identification of additional signs of “overdrive” in the 20 L chamber using the example of non-explosive anthracite to reduce the probability of the above-mentioned qualitative error.</p></sec><sec><title>Analysis of publications</title><p>Analysis of publications. The random nature of anthracite explosiveness over a wide range of dust concentrations at Eig = 5 kJ was observed (Cashdollar, Chatrathi, 1993). Two inflection points on the ascending branch of the dependence of the anthracite explosion pressure P on time t are observed, corresponding first to the minimum and then to the maximum dP/dt, respectively. All these features may be signs of “overdrive” after experimental testing.</p><p>Anthracite and its research method. Anthracite with the volatile content of 2.7 % wt. was studied in a 20 L. Siwek chamber, Eig = 10 kJ, with video recording of radiation through an observation window.</p></sec><sec><title>Results</title><p>Results. Time dependences of the medium radiation intensity and the pressure in the chamber on time in the range of dust concentrations from 125 to 750 g/m3 are obtained.</p><p>Discussion and conclusions. Three additional signs of the “overdrive” effect for anthracite were confirmed experi­mentally and proposed: probabilistic nature of the explosion hazard; two inflection points on the ascending branch of the graph P(t); noticeable weakening of the medium radiation after the ignition source burnout and before reaching the lower inflection point. The explosion pressure exceeded 400 kPa and was mainly caused by the burning of fixed carbon.</p></sec></trans-abstract><kwd-group xml:lang="ru"><kwd>уголь</kwd><kwd>взрывоопасность</kwd><kwd>камера Сивека</kwd><kwd>признаки «overdrive»</kwd><kwd>свечение пламени</kwd></kwd-group><kwd-group xml:lang="en"><kwd>coal</kwd><kwd>explosion hazard</kwd><kwd>Siwek chamber</kwd><kwd>overdrive signs</kwd><kwd>flame glow</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">Eckhoff R.K. Dust explosions in the process industries : 3rd ed. Boston : Gulf Professional Publishing/Elsevier, 2003. 720 p.</mixed-citation><mixed-citation xml:lang="en">Eckhoff R.K. Dust explosions in the process industries: 3rd ed. Gulf Professional Publishing/Elsevier. 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