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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="en"><front><journal-meta><journal-id journal-id-type="publisher-id">najo</journal-id><journal-title-group><journal-title xml:lang="en">Nanosystems: Physics, Chemistry, Mathematics</journal-title><trans-title-group xml:lang="ru"><trans-title>Наносистемы: физика, химия, математика</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">2220-8054</issn><issn pub-type="epub">2305-7971</issn><publisher><publisher-name>Университет ИТМО</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.17586/2220-8054-2015-6-3-366-377</article-id><article-id custom-type="elpub" pub-id-type="custom">najo-995</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="en"><subject>PHYSICS</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="ru"><subject>ФИЗИКА</subject></subj-group></article-categories><title-group><article-title>Statistical mechanics of transport processes of fluids under confined conditions</article-title><trans-title-group xml:lang="ru"><trans-title></trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="western" xml:lang="en"><surname>Rudyak</surname><given-names>V.</given-names></name></name-alternatives><bio xml:lang="en"><p>Novosibirsk</p></bio><email xlink:type="simple">valery.rudyak@mail.ru</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="western" xml:lang="en"><surname>Belkin</surname><given-names>A.</given-names></name></name-alternatives><bio xml:lang="en"><p>Novosibirsk</p></bio><email xlink:type="simple">a.belkin@ngs.ru</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff xml:lang="en" id="aff-1"><institution>Novosibirsk State University of Architecture and Civil Engineering</institution><country>Russian Federation</country></aff><pub-date pub-type="collection"><year>2015</year></pub-date><pub-date pub-type="epub"><day>15</day><month>08</month><year>2025</year></pub-date><volume>6</volume><issue>3</issue><fpage>366</fpage><lpage>377</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Rudyak V., Belkin A., 2025</copyright-statement><copyright-year>2025</copyright-year><copyright-holder xml:lang="ru">Rudyak V., Belkin A.</copyright-holder><copyright-holder xml:lang="en">Rudyak V., Belkin 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://nanojournal.ifmo.ru/jour/article/view/995">https://nanojournal.ifmo.ru/jour/article/view/995</self-uri><abstract><p>The problem of adequately describing transport processes of fluids in confined conditions is solved using methods of nonequilibrium statistical mechanics. The ‘fluid–channel wall’ system is regarded as a two-fluid medium, in which each phase has a particular velocity and temperature. The obtained results show that the transport equations in confined spaces should contain not only the stress tensor and the heat flux vector, but also the interfacial forces responsible for the transfer of momentum and heat due to the interaction with the wall surfaces. The stress tensor and the heat flux vector fluid can be expressed in terms of the effective viscosity and thermal conductivity. However, the constitutive relations contain additive terms that correspond to fluid–surface interactions. Thus, not only do the fluid transport coefficients in nanochannels differ from the bulk transport coefficients, but they are also not only determined by the parameters of the fluid.</p></abstract><kwd-group xml:lang="en"><kwd>Micro flow</kwd><kwd>transport coefficients</kwd><kwd>nonequilibrium statistical mechanics</kwd><kwd>confined system</kwd></kwd-group><funding-group><funding-statement xml:lang="en">This work was supported in part by the Russian Scientific Foundation (Grant No. 14 19-00312).</funding-statement></funding-group></article-meta></front><back><ref-list><title>References</title><ref id="cit1"><label>1</label><citation-alternatives><mixed-citation xml:lang="ru">Andryushchenko V., Rudyak V. Self-diffusion coefficient of molecular fluid in porous media. Defect and Diffusion Forum, 2011, 312–315, P. 417–422.</mixed-citation><mixed-citation xml:lang="en">Andryushchenko V., Rudyak V. Self-diffusion coefficient of molecular fluid in porous media. 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