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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">mireabulletin</journal-id><journal-title-group><journal-title xml:lang="ru">Russian Technological Journal</journal-title><trans-title-group xml:lang="en"><trans-title>Russian Technological Journal</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">2782-3210</issn><issn pub-type="epub">2500-316X</issn><publisher><publisher-name>RTU MIREA</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.32362/2500-316X-2021-9-5-57-66</article-id><article-id custom-type="elpub" pub-id-type="custom">mireabulletin-368</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>МАТЕМАТИЧЕСКОЕ МОДЕЛИРОВАНИЕ</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>MATHEMATICAL MODELING</subject></subj-group></article-categories><title-group><article-title>Испарение жидкой лежащей капли в условиях вынужденной конвекции</article-title><trans-title-group xml:lang="en"><trans-title>Evaporation of a liquid sessile droplet subjected to forced convection</trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0002-3413-8855</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Коренченко</surname><given-names>А. Е.</given-names></name><name name-style="western" xml:lang="en"><surname>Korenchenko</surname><given-names>A. Е.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Коренченко Анна Евгеньевна, д.ф.-м.н., профессор, кафедра высшей математики Института комплексной безопасности и специального приборостроения</p><p>119454, Москва, пр-т Вернадского, д. 78</p><p>Scopus Author ID 10043443100</p></bio><bio xml:lang="en"><p>Anna E. Korenchenko, Dr. Sci. (Phys.-Math.), Professor, Department of High Mathematics, Institute of Integrated Safety and Special Instrument Engineering</p><p>78, Vernadskogo pr.,  Moscow,  119454  </p><p>Scopus Author ID 10043443100</p></bio><email xlink:type="simple">korenchenko@mirea.ru</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0003-4511-1882</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Жукова</surname><given-names>А. А.</given-names></name><name name-style="western" xml:lang="en"><surname>Zhukova</surname><given-names>A. A.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Жукова Анна Александровна, к.х.н., доцент, кафедра аналитической, физической и коллоидной химии</p><p>105043, Москва, 5-ая Парковая ул., 21</p><p>Scopus Author ID 12757009400</p></bio><bio xml:lang="en"><p>Anna A. Zhukova, Cand. Sci. (Chem.), Associate Professor</p><p>21, 5 Parkovaya ul., Moscow, 105043</p><p>Scopus Author ID 12757009400</p></bio><email xlink:type="simple">anyazhu@gmail.com</email><xref ref-type="aff" rid="aff-2"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>«МИРЭА – Российский технологический университет»</institution><country>Россия</country></aff><aff xml:lang="en"><institution>MIREA – Russian Technological University</institution><country>Russian Federation</country></aff></aff-alternatives><aff-alternatives id="aff-2"><aff xml:lang="ru"><institution>Первый Московский государственный медицинский университет им. И.М. Сеченова </institution><country>Россия</country></aff><aff xml:lang="en"><institution>Sechenov First Moscow State Medical University</institution><country>Russian Federation</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2021</year></pub-date><pub-date pub-type="epub"><day>25</day><month>10</month><year>2021</year></pub-date><volume>9</volume><issue>5</issue><fpage>57</fpage><lpage>66</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Коренченко А.Е., Жукова А.А., 2021</copyright-statement><copyright-year>2021</copyright-year><copyright-holder xml:lang="ru">Коренченко А.Е., Жукова А.А.</copyright-holder><copyright-holder xml:lang="en">Korenchenko A.Е., Zhukova A.A.</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.rtj-mirea.ru/jour/article/view/368">https://www.rtj-mirea.ru/jour/article/view/368</self-uri><abstract><p>Результаты экспериментов по измерению скорости испарения с поверхности жидкой лежащей капли в воздух указывают, что конвективные потоки над поверхностью увеличивают скорость испарения. Однако данные относительно того, в какой мере конвекция влияет на процесс испарения, сильно разнятся, часто противоречивы и требуют уточнения. В работе проведен численный анализ испарения с поверхности капли воды в нейтральный газ – воздух в присутствии конвективных течений в газовой фазе. Капля располагается на горизонтальной, гладкой, изотермической подложке, рассмотрена мода с постоянным углом смачивания. Задача решена в осесимметричном приближении, течения вынужденной конвекции, совместимые с условиями симметрии, представлены потоками, направленными вниз вдоль оси системы и расходящимися по сторонам вблизи капли и подложки. Математическая модель учитывает влияние сил поверхностного натяжения, тяготения и вязкости в обеих средах, возможную свободную гравитационную конвекцию в газовой и жидкой средах, конвекцию Марангони в капле и построена для испарения, контролируемого диффузией в газовой фазе. Получены результаты, свидетельствующие о взаимном влиянии жидкой и газовой сред: капля колеблется под влиянием движений в атмосфере, что порождает волну плотности в газе: колеблющаяся капля «звучит». Величина скорости в жидкой среде в 50 раз меньше характерной скорости в воздухе. Обнаружено, что скорость испарения не изменяется в присутствии течений вынужденной конвекции, что противоречит большинству экспериментальных работ. Предположительная причина расхождений заключается в возникновении неравновесных условий на границе конденсированной фазы, при которых режим испарения перестает быть диффузионным.</p></abstract><trans-abstract xml:lang="en"><p>Experiments on measuring the rate of evaporation of liquid sessile droplets into air show that the rate of evaporation increases in the presence of forced convection flows. However, data on the effect of convection on evaporation are often contradictory and should be clarified. The paper presents a numerical analysis of evaporation from the surface of a water droplet subjected to forced convection in the gas phase. The drop is located on a smooth horizontal isothermal substrate; the mode with constant contact angle is considered. The shape of the drop has axial symmetry, the same for the velocities and pressure. Forced convection compatible with the symmetry conditions are represented by flows directed downward along the axis of the system and diverging along the sides near the drop and the substrate. The mathematical model is constructed for evaporation controlled by diffusion in the gas phase and takes into account surface tension, gravity, and viscosity in both media, buoyancy and Marangoni convection. The results indicate the existence of the mutual influence of liquid and gaseous media. Thus, a drop vibrates under the influence of movements in the atmosphere, which generates a density wave in the gas: the drop «sounds». The magnitude of the velocity in a liquid is 50 times less than the characteristic velocity in air. It is found that the evaporation rate does not change in the presence of forced convection flows, which contradicts most of the experimental works. The reason for the discrepancies is supposed to be the appearance of nonequilibrium conditions at the boundary of the condensed phase: under these conditions, the evaporation regime ceases to be diffusional.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>испарение</kwd><kwd>диффузия</kwd><kwd>лежащая капля</kwd><kwd>вынужденная конвекция</kwd><kwd>численное моделирование</kwd></kwd-group><kwd-group xml:lang="en"><kwd>evaporation</kwd><kwd>diffusion</kwd><kwd>sessile droplet</kwd><kwd>forced convection</kwd><kwd>mathematical modeling</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">Borodulin V.Y., Letushko V.N., Nizovtsev M.I., Sterlyagov A.N. 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