<?xml version='1.0' encoding='UTF-8'?><?xml-stylesheet href='static/style.xsl' type='text/xsl'?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-05-02T13:16:23Z</responseDate><request verb="GetRecord" identifier="oai:ebiltegia.mondragon.edu:20.500.11984/5885" metadataPrefix="rdf">https://ebiltegia.mondragon.edu/oai/request</request><GetRecord><record><header><identifier>oai:ebiltegia.mondragon.edu:20.500.11984/5885</identifier><datestamp>2024-03-04T13:48:23Z</datestamp><setSpec>com_20.500.11984_473</setSpec><setSpec>col_20.500.11984_478</setSpec></header><metadata><rdf:RDF xmlns:rdf="http://www.openarchives.org/OAI/2.0/rdf/" xmlns:ow="http://www.ontoweb.org/ontology/1#" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:ds="http://dspace.org/ds/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/rdf/ http://www.openarchives.org/OAI/2.0/rdf.xsd">
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      <dc:title>Pattern selection for convective flow in a liquid bridge subjected to remote thermal action</dc:title>
      <dc:creator>Shevtsova, Valentina</dc:creator>
      <dc:contributor>Gaponenko, Yuri</dc:contributor>
      <dc:contributor>Yano, Takeru</dc:contributor>
      <dc:contributor>Nishino, Kazuyoshi</dc:contributor>
      <dc:contributor>Matsumoto, Shuji</dc:contributor>
      <dc:description>The stability of thermocapillary/buoyant flows is affected by a remote thermal source. We present a nonlinear two-phase computational study of convection in a liquid bridge that develops under the action of Marangoni and buoyancy forces as well as under the influence of distant thermal disturbances. The gas phase (air) occupies a typical annular container holding a liquid bridge (n-decane, Pr = 14), and the disturbances are locally imposed in the form of hot/cold spots on the outer wall of the container. The hydrothermal wave instability and pattern selection have been explored for two temperature differences Δ𝑇���� by varying the intensity of thermal source Hf over a wide range. Not far from the critical point, in all the cases, the instability emerges in the form of a standing wave, but the azimuthal wavenumber depends on whether the external perturbation is caused by cooling (m = 2) or by heating (m = 1). Further into supercritical area, 45% above the threshold, in the region with thermal perturbations ⎯200&lt;𝐻����𝑓����&lt;50, the flow pattern comprises, but is not limited to, a hydrothermal traveling wave with the azimuthal wavenumber m = 2. For hotter perturbations, the instability develops either in the form of traveling or standing waves, depending on Hf, with the prevailing mode m = 1, but with a strong presence of other modes.</dc:description>
      <dc:date>2022-11-24T14:47:16Z</dc:date>
      <dc:date>2022-11-24T14:47:16Z</dc:date>
      <dc:date>2022</dc:date>
      <dc:type>http://purl.org/coar/resource_type/c_6501</dc:type>
      <dc:identifier>1089-7666</dc:identifier>
      <dc:identifier>https://katalogoa.mondragon.edu/janium-bin/janium_login_opac.pl?find&amp;ficha_no=169047</dc:identifier>
      <dc:identifier>https://hdl.handle.net/20.500.11984/5885</dc:identifier>
      <dc:language>eng</dc:language>
      <dc:rights>© 2022 AIP Publishing</dc:rights>
      <dc:publisher>AIP Publishing</dc:publisher>
   </ow:Publication>
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