<?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>2026-04-17T07:38:23Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2117/121985" metadataPrefix="marc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2117/121985</identifier><datestamp>2026-01-15T05:25:37Z</datestamp><setSpec>com_2072_1033</setSpec><setSpec>col_2072_452950</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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      <subfield code="a">Knops, Robin J.</subfield>
      <subfield code="e">author</subfield>
   </datafield>
   <datafield ind2=" " ind1=" " tag="720">
      <subfield code="a">Quintanilla de Latorre, Ramón</subfield>
      <subfield code="e">author</subfield>
   </datafield>
   <datafield ind2=" " ind1=" " tag="260">
      <subfield code="c">2018-12</subfield>
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      <subfield code="a">Zanaboni's procedure for establishing Saint-Venant's principle is ex-&#xd;
tended to anisotropic homogeneous transient heat conduction on regions&#xd;
that are successively embedded in each other to become indefinitely elon-&#xd;
gated. No further geometrical restrictions are imposed. The boundary&#xd;
of each region is maintained at zero temperature apart from the common&#xd;
surface of intersection which is heated to the same temperature assumed&#xd;
to be of bounded time variation. Heat sources are absent. Subject to&#xd;
these conditions, the thermal energy, supposed bounded in each region,&#xd;
becomes vanishingly small in those parts of the regions suficiently remote&#xd;
from the heated common surface. As with the original treatment, the&#xd;
proof involves certain monotone bounded sequences, and does not depend&#xd;
upon differential inequalities or the maximum principle. A definition is&#xd;
presented of an elongated region.</subfield>
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      <subfield code="a">Postprint (author's final draft)</subfield>
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      <subfield code="a">Àrees temàtiques de la UPC::Matemàtiques i estadística::Matemàtica aplicada a les ciències</subfield>
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      <subfield code="a">Heat--Conduction</subfield>
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      <subfield code="a">Differential equations, Partial</subfield>
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      <subfield code="a">Calor -- Conducció</subfield>
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      <subfield code="a">Equacions diferencials parcials</subfield>
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      <subfield code="a">Classificació AMS::58 Global analysis, analysis on manifolds::58J Partial differential equations on manifolds; differential operators</subfield>
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      <subfield code="a">Classificació AMS::80 Classical thermodynamics, heat transfer</subfield>
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   <datafield ind2="0" ind1="0" tag="245">
      <subfield code="a">Spatial decay in transient heat conduction for general elongated regions</subfield>
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