Solving the heat equation with variable thermal conductivity
We consider the heat equation with spatially variable thermal conductivity and homogeneous Dirichlet boundary conditions. Using the Method of Fokas or Unified Transform Method, we derive solution representations as the limit of solutions of constant-coefficient interface problems where the number of...
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creator | Farkas, Matthew Deconinck, Bernard |
description | We consider the heat equation with spatially variable thermal conductivity
and homogeneous Dirichlet boundary conditions. Using the Method of Fokas or
Unified Transform Method, we derive solution representations as the limit of
solutions of constant-coefficient interface problems where the number of
subdomains and interfaces becomes unbounded. This produces an explicit
representation of the solution, from which we can compute the solution and
determine its properties. Using this solution expression, we can find the
eigenvalues of the corresponding variable-coefficient eigenvalue problem as
roots of a transcendental function. We can write the eigenfunctions explicitly
in terms of the eigenvalues. The heat equation is the first example of more
general variable-coefficient second-order initial-boundary value problems that
can be solved using this approach. |
doi_str_mv | 10.48550/arxiv.2208.01764 |
format | Article |
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and homogeneous Dirichlet boundary conditions. Using the Method of Fokas or
Unified Transform Method, we derive solution representations as the limit of
solutions of constant-coefficient interface problems where the number of
subdomains and interfaces becomes unbounded. This produces an explicit
representation of the solution, from which we can compute the solution and
determine its properties. Using this solution expression, we can find the
eigenvalues of the corresponding variable-coefficient eigenvalue problem as
roots of a transcendental function. We can write the eigenfunctions explicitly
in terms of the eigenvalues. The heat equation is the first example of more
general variable-coefficient second-order initial-boundary value problems that
can be solved using this approach.</description><identifier>DOI: 10.48550/arxiv.2208.01764</identifier><language>eng</language><subject>Mathematics - Analysis of PDEs</subject><creationdate>2022-08</creationdate><rights>http://creativecommons.org/licenses/by/4.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,885</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/2208.01764$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.2208.01764$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Farkas, Matthew</creatorcontrib><creatorcontrib>Deconinck, Bernard</creatorcontrib><title>Solving the heat equation with variable thermal conductivity</title><description>We consider the heat equation with spatially variable thermal conductivity
and homogeneous Dirichlet boundary conditions. Using the Method of Fokas or
Unified Transform Method, we derive solution representations as the limit of
solutions of constant-coefficient interface problems where the number of
subdomains and interfaces becomes unbounded. This produces an explicit
representation of the solution, from which we can compute the solution and
determine its properties. Using this solution expression, we can find the
eigenvalues of the corresponding variable-coefficient eigenvalue problem as
roots of a transcendental function. We can write the eigenfunctions explicitly
in terms of the eigenvalues. The heat equation is the first example of more
general variable-coefficient second-order initial-boundary value problems that
can be solved using this approach.</description><subject>Mathematics - Analysis of PDEs</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNotj7tOwzAARb0woMIHMOEfSPAjjm2pC6p4SZU60D26frSxlCZg3ED_HrUwneFKR_cQcsdZ3Ril2APyT5prIZipGddtc02W79Mwp3FPSx9pH1Fo_DyipGmk36n0dEZOcEM87_mAgfppDEdf0pzK6YZc7TB8xdt_Lsj2-Wm7eq3Wm5e31eO6QqubSjMnRPCNBWSrWxmcsTxyZ6ClUrCKC8m8F8rz6GG5hbEa2CnmYvABckHu_7SX-91HTgfkU3fO6C4Z8hc1f0Ng</recordid><startdate>20220802</startdate><enddate>20220802</enddate><creator>Farkas, Matthew</creator><creator>Deconinck, Bernard</creator><scope>AKZ</scope><scope>GOX</scope></search><sort><creationdate>20220802</creationdate><title>Solving the heat equation with variable thermal conductivity</title><author>Farkas, Matthew ; Deconinck, Bernard</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a674-70b22dc49aa36763db891e1b8a7355a951230cc25c1eca919a897aaf50bedcda3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Mathematics - Analysis of PDEs</topic><toplevel>online_resources</toplevel><creatorcontrib>Farkas, Matthew</creatorcontrib><creatorcontrib>Deconinck, Bernard</creatorcontrib><collection>arXiv Mathematics</collection><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Farkas, Matthew</au><au>Deconinck, Bernard</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Solving the heat equation with variable thermal conductivity</atitle><date>2022-08-02</date><risdate>2022</risdate><abstract>We consider the heat equation with spatially variable thermal conductivity
and homogeneous Dirichlet boundary conditions. Using the Method of Fokas or
Unified Transform Method, we derive solution representations as the limit of
solutions of constant-coefficient interface problems where the number of
subdomains and interfaces becomes unbounded. This produces an explicit
representation of the solution, from which we can compute the solution and
determine its properties. Using this solution expression, we can find the
eigenvalues of the corresponding variable-coefficient eigenvalue problem as
roots of a transcendental function. We can write the eigenfunctions explicitly
in terms of the eigenvalues. The heat equation is the first example of more
general variable-coefficient second-order initial-boundary value problems that
can be solved using this approach.</abstract><doi>10.48550/arxiv.2208.01764</doi><oa>free_for_read</oa></addata></record> |
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subjects | Mathematics - Analysis of PDEs |
title | Solving the heat equation with variable thermal conductivity |
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