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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">cheb</journal-id><journal-title-group><journal-title xml:lang="ru">Чебышевский сборник</journal-title><trans-title-group xml:lang="en"><trans-title>Chebyshevskii Sbornik</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">2226-8383</issn><publisher><publisher-name>Tula State Lev Tolstoy  Pedagogical University</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.22405/2226-8383-2017-18-3-439-460</article-id><article-id custom-type="elpub" pub-id-type="custom">cheb-370</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>Статьи</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>Article</subject></subj-group></article-categories><title-group><article-title>МЕТОД ПОДВИЖНЫХ КЛЕТОЧНЫХ АВТОМАТОВ КАК НАПРАВЛЕНИЕ ДИСКРЕТНОЙ ВЫЧИСЛИТЕЛЬНОЙ МЕХАНИКИ</article-title><trans-title-group xml:lang="en"><trans-title>MOVABLE CELLULAR AUTOMATON METHOD AS A TREND IN DISCRETE COMPUTATIONAL MECHANICS</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>Псахье</surname><given-names>С. Г.</given-names></name><name name-style="western" xml:lang="en"><surname>Psakhie</surname><given-names>S. G.</given-names></name></name-alternatives><bio xml:lang="ru"><p>доктор физико-математических наук, профессор, член-корреспондент Российской академии наук, директор</p></bio><bio xml:lang="en"><p>doctor of physics and mathematics, professor, corresponding member of the Russian Academy of Sciences director</p></bio><email xlink:type="simple">sp@ispms.tsc.ru</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>Смолин</surname><given-names>А. Ю.</given-names></name><name name-style="western" xml:lang="en"><surname>Smolin</surname><given-names>A. Yu.</given-names></name></name-alternatives><bio xml:lang="ru"><p>доктор физико-математических наук, профессор, главный научный сотрудник</p></bio><bio xml:lang="en"><p>Doctor of physics and mathematics, Assistant professor Leader researcher </p></bio><email xlink:type="simple">asmolin@ispms.tsc.ru</email><xref ref-type="aff" rid="aff-2"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Дмитриев</surname><given-names>А. И.</given-names></name><name name-style="western" xml:lang="en"><surname>Dmitriev</surname><given-names>A. I.</given-names></name></name-alternatives><bio xml:lang="ru"><p>доктор физико-математических наук, доцент, ведущий научный сотрудник </p></bio><bio xml:lang="en"><p>Doctor of physics and mathematics, Assistant professor, Leader researcher</p></bio><email xlink:type="simple">dmitr@ispms.tsc.ru</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>Шилько</surname><given-names>Е. В.</given-names></name><name name-style="western" xml:lang="en"><surname>Shilko</surname><given-names>E. V.</given-names></name></name-alternatives><bio xml:lang="en"><p>Doctor of physics and mathematics, Assistant professor Deputy director </p></bio><email xlink:type="simple">shilko@ispms.tsc.ru</email><xref ref-type="aff" rid="aff-3"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Коростелев</surname><given-names>С. Ю.</given-names></name><name name-style="western" xml:lang="en"><surname>Korostelev</surname><given-names>S. Yu.</given-names></name></name-alternatives><bio xml:lang="ru"><p>кандидат физико-математических наук, старший научный сотрудник </p></bio><bio xml:lang="en"><p>candidat of physics and mathematics, senior researcher</p></bio><email xlink:type="simple">sergeyk@ispms.tsc.ru</email><xref ref-type="aff" rid="aff-2"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Институт физики прочности и материаловедения Сибирского отделения РАН</institution><country>Россия</country></aff><aff xml:lang="en"><institution>Institute of Strength Physics and Materials Science of Siberian Branch of RAS</institution><country>Russian Federation</country></aff></aff-alternatives><aff-alternatives id="aff-2"><aff xml:lang="ru"><institution>Институт физики прочности и материаловедения Сибирского отделения РАН</institution><country>Россия</country></aff><aff xml:lang="en"><institution>Institute of Strength Physics and Materials Science of Siberian Branch of Russian Academy of Sciences</institution><country>Russian Federation</country></aff></aff-alternatives><aff xml:lang="en" id="aff-3"><institution>Institute of Strength Physics and Materials Science of Siberian Branch of RAS</institution><country>Russian Federation</country></aff><pub-date pub-type="collection"><year>2017</year></pub-date><pub-date pub-type="epub"><day>09</day><month>01</month><year>2018</year></pub-date><volume>18</volume><issue>3</issue><fpage>439</fpage><lpage>460</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Псахье С.Г., Смолин А.Ю., Дмитриев А.И., Шилько Е.В., Коростелев С.Ю., 2017</copyright-statement><copyright-year>2017</copyright-year><copyright-holder xml:lang="ru">Псахье С.Г., Смолин А.Ю., Дмитриев А.И., Шилько Е.В., Коростелев С.Ю.</copyright-holder><copyright-holder xml:lang="en">Psakhie S.G., Smolin A.Y., Dmitriev A.I., Shilko E.V., Korostelev 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://www.chebsbornik.ru/jour/article/view/370">https://www.chebsbornik.ru/jour/article/view/370</self-uri><abstract><p>В статье рассмотрены основные положения метода подвижных клеточных автоматов,  который предназначен для моделирования процессов деформирования и разрушения  материалов и сред в рамках метода частиц на различных масштабах. Изначально метод  частиц в механике материалов применялся только для моделирования поведения материалов на микроуровне в виде метода молекулярной динамики. Дальнейшее  его развитие привело к целой группе методов под общим названием метода дискретных  элементов, которые в основном применяются для моделирования сыпучих и  гранулированных материалов на макроуровне. Рассматриваемый в работе метод подвижных  клеточных автоматов разработан для моделирования процессов деформирования и  разрушения материалов на различных масштабах: на мезоскопическом масштабе с явным  учётом структуры материала и на макроскопическом масштабе в рамках среды с  эффективными свойствами. В работе изложены важные отличия и преимущества данного  подхода по сравнению с другими методами современной дискретной вычислительной механики. Эти преимущества обусловлены прежде всего тем, что представленный здесь  подход основывается на двух базовых методах дискретного моделирования: методе частиц  и методе клеточных автоматов. Использование формализма клеточных автоматов позволяет  явно описывать как процессы зарождения и развития повреждений (разрушения), так и  залечивания трещин и микросварки. Кроме того, в рамках этого же формализма возможно  описание процессов теплопроводности, химических и фазовых превращений. Вторым  важным преимуществом метода подвижных клеточных автоматов является многочастичный  характер взаимодействия его элементов. В результате использования многочастичного взаимодействия удаётся избавиться от искусственного влияния упаковки частиц и  локальности их взаимодействия в точках контакта на поведение моделируемого материала,  что наиболее важно для моделирования его упруго-пластического течения. В плане  дальнейшего развития рассмотренного подхода в работе предложены способы описания в  рамках метода частиц контактного взаимодействия поверхностей различных тел на микро- и мезоскопическом масштабах.</p></abstract><trans-abstract xml:lang="en"><p>The paper presents the basics of movable cellular automaton methodaimed for simulating deformation and fracture of materials and media at different scales. Initially, the particle method has been  employed in mechanics of materials only at microscale as molecular  dynamics. Its further development has been led to a group of  methods which are usually called as discrete element method and  used for simulation of loose and granular materials at the  macroscale. The presented method of movable cellular automata  was developed for simulating deformation and fracture of materials  at different scales: at mesoscale with an explicit account for material structure, and at macroscale within the framework of a media with effective properties. The main advantages and differences of  the approach compared with the other methods of discrete  computational mechanics are considered. These advantages, first of all, are determined by the fact that the considered approach is based on two basic methods of discrete simulation: particle method and  cellular automaton method. Employing the formalism of cellular  automata allows explicit description of both processes of damage  generation and evolution as well as of crack healing and  microwelding. More of that, it is possible to describe heat transfer, chemical reactions and phase transitions as well. The second  important advantage of the movable cellular automaton method is the many-body type of interaction among its elements. The use of  many-body interaction allows us to avoid artificial effect of the  particle packing and locality of their interaction on the resulting  behavior of the modeled material that is extremely important for  modeling elastic-plastic matereials. As a further development of the  considered approach, two techniques are discussed which enable to describe contact interaction of solid bodies surfaces at the microand mesoscopic scales within the framework of the particle method.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>вычислительная механика</kwd><kwd>метод частиц</kwd><kwd>клеточные автоматы</kwd><kwd>деформация и разрушение</kwd></kwd-group><kwd-group xml:lang="en"><kwd>computational mechanics</kwd><kwd>particle method</kwd><kwd>cellular automata</kwd><kwd>deformation and fracture</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">Darrigol O. Between hydrodynamics and elasticity theory: the first five births of the Navier-Stokes equation // Arch. Hist. Exact Sci. 2002. Vol. 56. 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