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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">sat</journal-id><journal-title-group><journal-title xml:lang="ru">НАУКА и ТЕХНИКА</journal-title><trans-title-group xml:lang="en"><trans-title>Science &amp; Technique</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">2227-1031</issn><issn pub-type="epub">2414-0392</issn><publisher><publisher-name>Belarusian National Technical University</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.21122/2227-1031-2025-24-4-270-277</article-id><article-id custom-type="elpub" pub-id-type="custom">sat-2876</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>МАШИНОСТРОЕНИЕ И МАШИНОВЕДЕНИЕ</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>MECHANICAL ENGINEERING АND ENGINEERING SCIENCE</subject></subj-group></article-categories><title-group><article-title>Изменение текстуры деформированной меди при воздействии холодной плазмы воздуха</article-title><trans-title-group xml:lang="en"><trans-title>Change in Texture of Deformed Copper Exposed to Cold Air Plasma</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>Анисович</surname><given-names>А. Г.</given-names></name><name name-style="western" xml:lang="en"><surname>Anisovich</surname><given-names>A. G.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Доктор физико-математических наук, профессор</p><p>Адрес для переписки:Анисович Анна Геннадиевна -Государственное научное учреждение «Институт прикладной физики Национальной академии наук Беларуси»ул. Академическая, 16,220072, г. Минск, Республика БеларусьТел.: +375 29 664-65-56аnna-anisovich@yandex.ru</p></bio><bio xml:lang="en"><p>Address for correspondence:Anisovich Anna G. -State Scientific Institution“Institute of Applied Physics of theNational Academy of Sciences of Belarus”16, Academic str.,220072, Minsk, Republic of BelarusTel.: +375 29 664-65-56аnna-anisovich@yandex.ru</p></bio><email xlink:type="simple">anna-anisovich@yandex.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>Филатова</surname><given-names>И. И.</given-names></name><name name-style="western" xml:lang="en"><surname>Filatova</surname><given-names>I. I.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Кандидат физико-математических наук, доцент</p><p>г. Минск</p></bio><bio xml:lang="en"><p>Minsk</p></bio><xref ref-type="aff" rid="aff-2"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Государственное научное учреждение «Институт прикладной физики Национальной академии наук Беларуси»</institution><country>Беларусь</country></aff><aff xml:lang="en"><institution>State Scientific Institution “Institute of Applied Physics of the National Academy of Sciences of Belarus”</institution><country>Belarus</country></aff></aff-alternatives><aff-alternatives id="aff-2"><aff xml:lang="ru"><institution>Государственное научное учреждение «Институт прикладной физики Национальной академии наук Беларуси»</institution><country>Беларусь</country></aff><aff xml:lang="en"><institution>State Scientific Institution “B. I. Stepanov Institute of Physics of the National Academy of Sciences of Belarus”</institution><country>Belarus</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2025</year></pub-date><pub-date pub-type="epub"><day>01</day><month>09</month><year>2025</year></pub-date><volume>24</volume><issue>4</issue><fpage>270</fpage><lpage>277</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Анисович А.Г., Филатова И.И., 2025</copyright-statement><copyright-year>2025</copyright-year><copyright-holder xml:lang="ru">Анисович А.Г., Филатова И.И.</copyright-holder><copyright-holder xml:lang="en">Anisovich A.G., Filatova I.I.</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://sat.bntu.by/jour/article/view/2876">https://sat.bntu.by/jour/article/view/2876</self-uri><abstract><p>Исследованы изменения микроструктуры и текстуры образцов меди М1 после пластической деформации прокаткой и воздействия низкотемпературной неравновесной плазмы высокочастотного емкостного разряда, возбуждаемого на частоте f = 5,28 МГц в воздухе при низком давлении (p ~ 1 Торр). Методом металлографического анализа показано, что изменения микроструктуры незначительны. Размер зерна не изменяется; улучшается визуализация структуры, повышается четкость выявления границ зерен после металлографического травления. Результаты рентгеноструктурного анализа свидетельствуют о том, что воздействие плазмы приводит к изменению относительной интенсивности интерференционных линий рентгенограммы. После деформации превалирующей является ориентировка á011ñ, что характерно для текстуры прокатки меди. Воздействие плазмы в течение 5 мин приводит к повышению интенсивности линий (200), (220) и (311). При обработке в течение 10 мин относительная интенсивность линий также незначительно возрастает. Параметр кристаллической решетки после воздействия плазмы не изменяется. Установлено, что изменение интенсивности линий рентгенограммы не связано с действием микронапряжений, изменением размеров блоков когерентного рассеяния. Значение отношения sinq(200)/sinq(111) = 1,15 свидетельствует о том, что дефекты упаковки в процессе воздействия не образуются. Рентгеновские эффекты при воздействии плазмы аналогичны наблюдаемым при отпуске деформированных металлов, когда основные ориентировки текстуры деформации или сохраняются на уровне деформированного металла, или усиливаются. При воздействии плазмы реализуется начальный процесс релаксации напряжений, связанный с перемещением атомов на расстояния, меньшие межатомных, когда кристаллическая решетка совершенствуется. Основной причиной изменений являются напряжения 3-го рода, обусловленные смещениями атомов из положений равновесия.</p></abstract><trans-abstract xml:lang="en"><p>The changes in the microstructure and texture of M1 copper samples after plastic deformation by rolling and exposure to low temperature non-equilibrium plasma of a high-frequency capacitive discharge excited at a frequency of f = 5.28 MHz in air at low pressure (p ~ 1 Torr) have been studied in the paper. The metallographic analysis showed that changes in the microstructure of samples are insignificant. The grain size does not change; the visualization of the structure is improved, and the clarity of detection of grain boundaries is increased after metallographic etching. The results of X-ray structural analysis showed that the effect of plasma treatment leads to a change in the relative intensity of the interference lines of the X-ray diffraction pattern. After deformation, the prevailing orientation is á011ñ, which is typical for the texture of copper rolling. After exposure to plasma for 5 minutes, the intensity of lines (200), (220) and (311) increases. A slight increase in the relative intensity of the lines is observed after plasma treatment for 10 minutes. The parameter of the crystal lattice does not change after exposure to plasma. It was found that the change in the intensity of the X-ray lines is not associated with the action of microstresses or a change in the size of coherent scattering blocks. The ratio sinq(200)/sinq(111) = 1.15 indicates that stacking faults are not formed during plasma treatment. X-ray effects under plasma exposure are similar to those observed during tempering of deformed metals, when the main orientations of the deformation texture are either maintained at the level of the deformed metal or are enhanced. Under plasma exposure, the initial process of stress relaxation is realized, associated with the movement of atoms over distances smaller than interatomic distances, when the crystal lattice is improved. The main reason of the changes is third-order stresses, caused by the displacement of atoms from their equilibrium positions.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>пластическая деформация</kwd><kwd>плазменная обработка</kwd><kwd>микроструктура</kwd><kwd>текстура</kwd><kwd>возврат напряжения</kwd><kwd>статические смещения атомов</kwd></kwd-group><kwd-group xml:lang="en"><kwd>plastic deformation</kwd><kwd>plasma treatment</kwd><kwd>microstructure</kwd><kwd>texture</kwd><kwd>recovery stress</kwd><kwd>static displacements of atoms</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">Review of the Cold Atmospheric Plasma Technology Application in Food, Disinfection, and Textiles: A Way Forward for Achieving Circular Economy / R. R. Reema [et al.] // Frontiers in Physics. 2022. 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