<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.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>2026-04-17T06:23:26Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2117/188825" metadataPrefix="marc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2117/188825</identifier><datestamp>2025-07-16T22:56:47Z</datestamp><setSpec>com_2072_1033</setSpec><setSpec>col_2072_452949</setSpec></header><metadata><record xmlns="http://www.loc.gov/MARC21/slim" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.loc.gov/MARC21/slim http://www.loc.gov/standards/marcxml/schema/MARC21slim.xsd">
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   <datafield ind2=" " ind1=" " tag="042">
      <subfield code="a">dc</subfield>
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   <datafield ind2=" " ind1=" " tag="720">
      <subfield code="a">Kawaguchi, Tatsuya</subfield>
      <subfield code="e">author</subfield>
   </datafield>
   <datafield ind2=" " ind1=" " tag="260">
      <subfield code="c">2013</subfield>
   </datafield>
   <datafield ind2=" " ind1=" " tag="520">
      <subfield code="a">For the stable melting of the high temperature molten glass beyond 1200 degree Celsius, ﬂuid motion and thermal energy balance due to the natural convection are the most important phenomena to control the state of the molten materials and blending process of the particulate materials. In the present study, the numerical simulation of natural convection ﬂow by the conductive heat transfer in a rectangular cavity was investigated. Moreover the eﬀect of the internal heating such as Joule heating was considered and compared, which was used in the engineering ﬁeld of the development of the glass melting method for vitriﬁed high-level radioactive waste. For the numerical analysis of the aforementioned ﬂow ﬁeld, the moving particle semi-implicit method was employed to predict the velocity distribution of the ﬂuid ﬂows as well as the temperature distribution. Mass, momentum and energy equation was used. Boussinesq approximation was applied to estimate the buoyancy force. Since the particle method we used is the meshless method, it is easy to compute the ﬂow with free surface as well as the throwing of the additional ﬂuid particles into the cavity. In the numerical analysis, Rayleigh number with internal heating was varied to compare the ﬂuid behaviour, spatial distribution of temperature and the velocity magnitude of the downward plume.</subfield>
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   <datafield tag="653" ind2=" " ind1=" ">
      <subfield code="a">Àrees temàtiques de la UPC::Matemàtiques i estadística::Anàlisi numèrica::Mètodes en elements finits</subfield>
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      <subfield code="a">Finite element method</subfield>
   </datafield>
   <datafield tag="653" ind2=" " ind1=" ">
      <subfield code="a">Computational methods in mechanics</subfield>
   </datafield>
   <datafield tag="653" ind2=" " ind1=" ">
      <subfield code="a">Particle methods (Numerical analysis)</subfield>
   </datafield>
   <datafield tag="653" ind2=" " ind1=" ">
      <subfield code="a">Natural convection, Internal heating, Molten glass, Particle Method</subfield>
   </datafield>
   <datafield tag="653" ind2=" " ind1=" ">
      <subfield code="a">Elements finits, Mètode dels</subfield>
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   <datafield ind2="0" ind1="0" tag="245">
      <subfield code="a">MPS simulation of natural convection with internal heating in a cavity</subfield>
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