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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">cvmet</journal-id><journal-title-group><journal-title xml:lang="ru">Известия вузов. Цветная металлургия</journal-title><trans-title-group xml:lang="en"><trans-title>Izvestiya. Non-Ferrous Metallurgy</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">0021-3438</issn><issn pub-type="epub">2412-8783</issn><publisher><publisher-name>НИТУ "МИСИС"</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.17073/0021-3438-2019-4-16-22</article-id><article-id custom-type="elpub" pub-id-type="custom">cvmet-991</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>Обработка металлов давлением</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>Pressure Treatment of Metals</subject></subj-group></article-categories><title-group><article-title>Исследование процесса уплотнения титансодержащей шихты экспериментально-аналитическим методом</article-title><trans-title-group xml:lang="en"><trans-title>Study of the process of titanium-containing furnace charging material compaction by an experimental-analytical method</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>Залазинский</surname><given-names>А. Г.</given-names></name><name name-style="western" xml:lang="en"><surname>Zalazinskii</surname><given-names>A. G.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Доктор технических наук, главный научный сотрудник лаборатории системного моделирования ИМАШ УрО РАН</p><p>620049, Екатеринбург, ул. Комсомольская, 34</p></bio><bio xml:lang="en"><p>Dr. Sci. (Tech.), Leading researcher, Laboratory of system simulation, IES UB RAS.</p><p>620049, Ekaterinburg, Komsomolskaya str., 34</p></bio><email xlink:type="simple">agz@imach.uran.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>Нестеренко</surname><given-names>А. В.</given-names></name><name name-style="western" xml:lang="en"><surname>Nesterenko</surname><given-names>A. V.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Кандидат технических наук, ст. научный сотрудник лаборатории микромеханики материалов ИМАШ УрО РАН.</p><p>620049, Екатеринбург, ул. Комсомольская, 34</p></bio><bio xml:lang="en"><p>Cand. Sci. (Tech.), Senior researcher, Laboratory of material micromechanics, IES UB RAS.</p><p>620049, Ekaterinburg, Komsomolskaya str., 34</p></bio><email xlink:type="simple">nav@imach.uran.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>Березин</surname><given-names>И. М.</given-names></name><name name-style="western" xml:lang="en"><surname>Berezin</surname><given-names>I. M.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Кандидат технических наук, научный сотрудник лаборатории системного моделирования ИМАШ УрО РАН; старший научный сотрудник УрФУ.</p><p>620002, Екатеринбург, ул. Мира, 19</p></bio><bio xml:lang="en"><p>Berezin I.M. — Cand. Sci. (Tech.), Researcher, Laboratory of system simulation, IES UB RAS; Senior researcher, UFU named after the first President of Russia B.N. Yeltsin.</p><p>620049, Ekaterinburg, Komsomolskaya str., 34</p></bio><email xlink:type="simple">berezin@imach.uran.ru</email><xref ref-type="aff" rid="aff-2"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Институт машиноведения, УрО РАН</institution><country>Россия</country></aff><aff xml:lang="en"><institution>Ural Branch of the Russian Academy of Sciences</institution><country>Russian Federation</country></aff></aff-alternatives><aff-alternatives id="aff-2"><aff xml:lang="ru"><institution>Институт машиноведения, УрО РАН; Уральский федеральный университет им. первого Президента России Б.Н. Ельцина</institution><country>Россия</country></aff><aff xml:lang="en"><institution>Ural Branch of the Russian Academy of Sciences; Ural Federal University named after the first President of Russia B.N. Yeltsin</institution><country>Russian Federation</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2019</year></pub-date><pub-date pub-type="epub"><day>14</day><month>08</month><year>2019</year></pub-date><volume>0</volume><issue>4</issue><fpage>16</fpage><lpage>22</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Залазинский А.Г., Нестеренко А.В., Березин И.М., 2019</copyright-statement><copyright-year>2019</copyright-year><copyright-holder xml:lang="ru">Залазинский А.Г., Нестеренко А.В., Березин И.М.</copyright-holder><copyright-holder xml:lang="en">Zalazinskii A.G., Nesterenko A.V., Berezin I.M.</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://cvmet.misis.ru/jour/article/view/991">https://cvmet.misis.ru/jour/article/view/991</self-uri><abstract><p>Исследована зависимость пористости порошкового материала на основе губчатого титана от коэффициента напряженного состояния в процессе пластического деформирования с преобладающим действием всестороннего сжатия. На основе результатов, полученных в предшествующих работах, на плоскости о—T построено семейство кривых текучести с варьируемой пористостью. Условие текучести порошкового материала основано на модели пластического течения Modified Drucker—Prager Cap model. На графике геометрической интерпретации принятого условия текучести нанесены прямые, соответствующие различным значениям коэффициента напряженного состояния k = σ/T, где σ — среднее гидростатическое напряжение, T — интенсивность касательных напряжений. Для формулировки связи пористости (θ,, %), среднего нормального напряжения (σ), выраженного в безразмерной форме, и коэффициента напряженного состояния (k) использованы точки пересечения семейства кривых, соответствующих образующим поверхностей текучести на плоскости σ —T, и радиальных прямых. В результате получено уравнение вида θ = θ (σ, k). Для проверки адекватности указанного соотношения выполнена экспериментальная часть исследования. Предварительно спрессованные при давлении 1000 МПа и температуре 325 °С порошковые заготовки подвергались электроэрозионной резке вдоль осевого сечения для получения плоских образцов (темплетов). На поверхности темплетов выбрано несколько характерных участков для определения локальной поверхностной пористости методом количественной металлографии. Дополнительно определялось напряженно-деформированное состояние в представительных участках путем численного моделирования. В зонах осевого сечения, соответствующих исследуемым областям, рассчитаны значения объемной пластической деформации, интенсивности касательных напряжений и среднего нормального напряжения. Показано, что коэффициент напряженного состояния при его варьировании в достаточно широком диапазоне (k = —10...—0,86) несущественно влияет на величину пористости.</p></abstract><trans-abstract xml:lang="en"><p>The study covers the dependence of spongy titanium-based powder material porosity on the stress state coefficient during plastic deformation with the prevailing effect of all-round compression. Based on the results obtained in previous papers, an assemblage of yield curves with varying porosity is constructed on the σ —T plane. The yielding condition of the powder material is based on the Modified Drucker—Prager Cap model. The graph of geometrical interpretation of the accepted yielding condition contains straight lines corresponding to different values of the stress state coefficient k = σ/T where о is the average hydrostatic stress, and T is the shear stress intensity. In order to formulate the relationship of porosity (θ, %), average normal stress (σ) expressed in the nondimensional form, and the stress state coefficient (k), intersection points of the yield curve assemblage corresponding to yield surface generatrices on the o—T plane and radial straight lines were used. As a result, an equation of the θ = θ(σ, k) form was obtained. The experimental part of the study was performed in order to test the adequacy of this ratio. Powder blanks pre-compacted at a pressure of 1000 MPa and a temperature of 325 °C were subjected to electrical discharge sawing along the axial section to obtain flat samples (templates). Several characteristic areas were selected on the surface of templates to determine local surface porosity using quantitative metallography. The stress-strain state in representative areas was additionally determined by numerical simulation. The calculated values of the volumetric plastic strain, shear stress intensity and average normal stress were determined in axial section zones corresponding to the studied areas. It is shown that the stress state coefficient varying within a sufficiently wide range (k = —10...—0.86) does not affect significantly the porosity value.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>компактирование</kwd><kwd>уплотнение</kwd><kwd>пористость</kwd><kwd>порошок</kwd><kwd>моделирование</kwd><kwd>модель текучести</kwd><kwd>коэффициент напряженного состояния</kwd></kwd-group><kwd-group xml:lang="en"><kwd>compaction</kwd><kwd>compression</kwd><kwd>porosity</kwd><kwd>powder</kwd><kwd>simulation</kwd><kwd>yield model</kwd><kwd>stress state 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">Нестеренко А.В., Новожонов В.И., Залазинский А.Г., Скрипов А.В. 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