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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">probener</journal-id><journal-title-group><journal-title xml:lang="ru">Известия высших учебных заведений. ПРОБЛЕМЫ ЭНЕРГЕТИКИ</journal-title><trans-title-group xml:lang="en"><trans-title>Power engineering: research, equipment, technology</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">1998-9903</issn><issn pub-type="epub">2658-5456</issn><publisher><publisher-name>Kazan State Power Engineering  University</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.30724/1998-9903-2018-20-3-4-136-144</article-id><article-id custom-type="elpub" pub-id-type="custom">probener-575</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>ФИЗИКА</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>PHYSICS</subject></subj-group></article-categories><title-group><article-title>ЭКСПЕРИМЕНТАЛЬНОЕ ОПРЕДЕЛЕНИЕ ТЕМПЕРАТУР В ХАРАКТЕРНЫХ СЕЧЕНИЯХ РАБОЧЕЙ ЗОНЫ ЗАМКНУТОГО ДВУХФАЗНОГО ТЕРМОСИФОНА</article-title><trans-title-group xml:lang="en"><trans-title>EXPERIMENTAL DETERMINATION OF TEMPERATURES IN CHARACTERISTIC SECTIONS OF THE WORKING ZONE OF A CLOSED TWO-PHASE THERMOSYPHON</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>Кузнецов</surname><given-names>Г. В.</given-names></name><name name-style="western" xml:lang="en"><surname>Kuznetsov</surname><given-names>G. V.</given-names></name></name-alternatives><bio xml:lang="ru"><p>д-р физ.-мат. наук, профессор, заведующий кафедрой «Теоретическая и промышленная теплотехника» Томского политехнического университета</p></bio><bio xml:lang="en"><p>Tomsk polytechnic university, Doctor of Physical - Mathematical Sciences, Head of Department of thermal theory and engineering</p></bio><email xlink:type="simple">marisha@tpu.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>Нурпейис</surname><given-names>А. Е.</given-names></name><name name-style="western" xml:lang="en"><surname>Nurpeiis</surname><given-names>A. E.</given-names></name></name-alternatives><bio xml:lang="ru"><p>ассистент кафедры «Теоретическая и промышленная теплотехника» Томского политехнического университета</p></bio><bio xml:lang="en"><p>Tomsk Polytechnic University, Department of thermal theory and engineering, assistant</p></bio><email xlink:type="simple">nurpeiis_atlant@mail.ru</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Национальный исследовательский Томский политехнический университет</institution><country>Россия</country></aff><aff xml:lang="en"><institution>Tomsk Polytechnic University</institution><country>Russian Federation</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2018</year></pub-date><pub-date pub-type="epub"><day>25</day><month>05</month><year>2018</year></pub-date><volume>20</volume><issue>3-4</issue><fpage>136</fpage><lpage>144</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Кузнецов Г.В., Нурпейис А.Е., 2018</copyright-statement><copyright-year>2018</copyright-year><copyright-holder xml:lang="ru">Кузнецов Г.В., Нурпейис А.Е.</copyright-holder><copyright-holder xml:lang="en">Kuznetsov G.V., Nurpeiis A.E.</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.energyret.ru/jour/article/view/575">https://www.energyret.ru/jour/article/view/575</self-uri><abstract><p>Представлены результаты экспериментального определения распределений температур в характерных сечениях рабочей зоны замкнутого двухфазного термосифона. Исследования процессов теплопереноса проводились в термосифоне, изготовленном из меди с постоянной площадью поперечного сечения. Высота теплообменника 161 мм, толщина боковых стенок 1,5 мм, нижней стенки 2мм, внутренний диаметр испарительной части и парового канала 39 мм. По результатам экспериментальных исследований установлена зависимость изменения характерных температур от величины теплового потока, подводимого к нижней крышке термосифона, и коэффициента заполнения. Установлено, что увеличение теплового потока на нижней крышке термосифона приводит к снижению перепада температур по паровому каналу и сокращению времени выхода на стационарный режим работы. Эксперименты показали, что даже при высоких тепловых нагрузках (до 11,2 кВт/м2) перепады температур по высоте термосифона не превышают 9 К.</p></abstract><trans-abstract xml:lang="en"><p>In article, presents the results of experimental determination of temperature distributions in characteristic sections of the working zone of a closed two-phase thermosyphon. A thermosyphon made of copper with a constant cross-sectional area is used to study heat transfer. The height of the heat exchanger is 161 mm, the thickness of the side walls is 1.5 mm, the bottom wall is 2 mm, the internal diameter of the evaporative part and the vapor channel is 39 mm. Experimental results give dependences of the change in the characteristic temperatures on the heat flux supplied to the bottom cover of the thermosyphon and the filling ratio. An increase in the heat flow at the bottom cover of the thermosyphon leads to a decrease in the temperature drop along the vapor channel and a reduction in the time to reach the stationary mode of operation. Experiments show that even at high thermal loads (up to 11,2  kW/m2) the temperature drops over the height of the thermosyphon do not exceed 9 K.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>двухфазный термосифон</kwd><kwd>тепловой поток</kwd><kwd>теплоперенос</kwd><kwd>испарение</kwd><kwd>конденсация</kwd><kwd>коэффициент заполнения</kwd></kwd-group><kwd-group xml:lang="en"><kwd>two-phase thermosyphon</kwd><kwd>heat flow</kwd><kwd>heat transfer</kwd><kwd>evaporation</kwd><kwd>condensation</kwd><kwd>filling ratio</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">Franco A., Filippeschi S. 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