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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">10.22227/0869-7493.2022.31.02.15-21</article-id><article-id custom-type="elpub" pub-id-type="custom">firesmi-1100</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>Об оценке взрывоопасности ядерного графита в 1-м3 камере</article-title><trans-title-group xml:lang="en"><trans-title>Explosibility of nuclear graphite measured in a 1 m3 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 ID: 1093620</p></bio><bio xml:lang="en"><p>Nikolay L. Poletaev, Dr. Sci. (Eng.), Leading Researcher</p><p>12, Balashikha, Moscow Region, 143903</p><p>ID RISC:1093620</p></bio><email xlink:type="simple">nlpvniipo@mail.ru</email><xref ref-type="aff" rid="aff-1"/></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><pub-date pub-type="collection"><year>2022</year></pub-date><pub-date pub-type="epub"><day>02</day><month>06</month><year>2022</year></pub-date><volume>31</volume><issue>2</issue><fpage>15</fpage><lpage>21</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Полетаев Н.Л., 2022</copyright-statement><copyright-year>2022</copyright-year><copyright-holder xml:lang="ru">Полетаев Н.Л.</copyright-holder><copyright-holder xml:lang="en">Poletaev N.L.</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/1100">https://www.fire-smi.ru/jour/article/view/1100</self-uri><abstract><sec><title>Введение</title><p>Введение. Ядерный графит представляет угрозу образования аэровзвеси пыли графита (АПГ) при демонтаже вышедших из эксплуатации ядерных реакторов. В то же время нет ясного ответа на вопрос о взрывоопасности АПГ. Согласно обзору международных исследований, взрывоопасность АПГ либо отсутствует, либо слабо выражена (Phylaktou H.N. и др., 2015). В настоящей работе приводятся аргументы в пользу мнения о взрывобезопасности АПГ.</p><p>Выбранный результат исследования. Рассматривался известный результат исследования горения АПГ со средним размером частиц 5 мкм и концентрацией около 450 г/м3 в камере объемом 1,138 м3 с источником зажигания фирмы Fr. Sobbe GmbH («Sobbe 10 kJ»). Максимальное избыточное давление ΔPmax в камере составило 0,47 бар, что в соответствии с EN 14034-3 отвечает случаю взрывоопасной аэровзвеси (1 бар = 100 кПа).</p><p>Интерпретация результата исследования. Проведено сравнение осциллограмм давления для двух случаев: случая максимального проявления взрывоопасности АПГ (ΔPmax = 0,47 бар; dP/dt|max = 3,8 бар/с) и случая срабатывания источника зажигания в отсутствие аэровзвеси (ΔPmax = 0,027 бар; dP/dt|max = 2,7 бар/с). Сопоставление показало, что первые 20 мс изменения давления в камере обусловлены, в основном, горением источника зажигания: характерные значения ΔP = 0,03 бар и (dP/dt) ≈ 3,8 бар/с близки к показателям горения «Sobbe 10 kJ» в отсутствие АПГ. Дальнейшее увеличение ΔP происходит при постоянном или резко убывающем значении (dP/dt), что означает монотонное снижение скорости пламени и выявляет негорючесть АПГ.</p></sec><sec><title>Выводы</title><p>Выводы. Ввиду малости ΔPmax рассмотренную АПГ возможно считать взрывобезопасной при нормальных атмосферных условиях. Графики зависимостей давления продуктов горения и скорости его нарастания от времени являются важными сведениями о горении аэровзвеси во взрывных камерах при низкой взрывоопасности пыли.</p></sec></abstract><trans-abstract xml:lang="en"><sec><title>Introduction</title><p>Introduction. Nuclear graphite poses a threat due to the formation of the graphite dust – air mixture (GDAM) during the dismantling of decommissioned nuclear reactors. However, there is no clear answer to the question on the GDAM explosibility. A review of international studies suggests that GDAM is either inexplosive or its explosibility is weak (Phylaktou H.N. et al., 2015). In this paper, the authors advance arguments for the explosion safety of GDAM.</p></sec><sec><title>Selected research result</title><p>Selected research result. The authors considered a well-known result of a study on the combustion of GDAM with an average particle size of 5 μm, the concentration of about 450 g/m3 in a 1.138 m3 chamber, and an ignitionsource made by Fr. Sobbe GmbH («Sobbe 10 kJ»). The maximum overpressure ΔPmax was 0.47 bar in the chamber, and it fitted the case of an explosive air suspension, according to EN 14034-3 (1 bar = 100 kPa).</p><p>Interpretation of the research result. Pressure oscillograms were compared for the following two cases: the case of the maximum manifestation of the GDAM explosion hazard (ΔPmax = 0.47 bar; dP/dt|max = 3.8 bar/s) and the case of combustion of an ignition source in the absence of air suspension (ΔPmax = 0.027 bar; dP/dt|max = 2.7 bar/s). The comparison shows that the first 20 ms of a pressure change inside the chamber is mainly due to the combustion of the ignition source: the characteristic values ΔP = 0.03 bar and (dP/dt) ≈ 3.8 bar/s are close to the «Sobbe 10kJ» combustion index in the absence of GDAM. A further increase in ΔP is accompanied by the constant or sharply decreasing value of (dP/dt), which means a monotonous decrease in the flame velocity and proves the incombustibility of GDAM.</p></sec><sec><title>Conclusions</title><p>Conclusions. Due to the smallness of ΔPmax, GDAM can be considered nonexplosive under normal atmospheric conditions. Dependency diagrams, relating the pressure of combustion products and its growth to time offer important information about the combustion of the air suspension in explosion chambers under the condition of a low dust explosion hazard.</p></sec></trans-abstract><kwd-group xml:lang="ru"><kwd>пыль графита</kwd><kwd>аэровзвесь</kwd><kwd>взрыв</kwd><kwd>осциллограмма давления</kwd><kwd>снижение скорости пламени</kwd></kwd-group><kwd-group xml:lang="en"><kwd>graphite dust</kwd><kwd>air suspension</kwd><kwd>explosion</kwd><kwd>pressure oscillogram</kwd><kwd>flame velocity reduction</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">Turkevich L.A., Dastidar A.G., Hachmeister Z., Lim M. Potential explosion hazard of carbonaceous nanoparticles: Explosion parameters of selected materials // Journal of Hazardous Materials. 2015. Vol. 295. Pp. 97–103. 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