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Further boundary conditions in heat conduction problems in multilayer structures
This paper presents an approximate analytical solution of the heat conduction problem for a two-layer plate under symmetric boundary conditions of the first kind. The solution was determined on the basis of the property of the parabolic heat transfer equation associated with an infinite velocity of...
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Published in: | Journal of physics. Conference series 2021-02, Vol.1745 (1), p.12073 |
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description | This paper presents an approximate analytical solution of the heat conduction problem for a two-layer plate under symmetric boundary conditions of the first kind. The solution was determined on the basis of the property of the parabolic heat transfer equation associated with an infinite velocity of heat propagation, by determining the accessory unknown function and accessory boundary conditions in the integral heat balance method.
Local coordinate systems are given in order to obtain the simplest possible coordinate system satisfying the matching conditions and boundary conditions for each separate layer. An accessory unknown function is the temperature change over time in the center of symmetry. The use of this function in the heat balance integral method allows for reduction in the solution of the initial partial differential equation to the integration of an ordinary differential equation with respect to the additional unknown function.
Further boundary conditions are defined in such a way that their satisfaction by an unknown solution is equivalent to the satisfaction of the equations at the boundary points. Studies have shown that the equation fulfillment at the boundaries leads to their fulfillment within the regions. |
doi_str_mv | 10.1088/1742-6596/1745/1/012073 |
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Local coordinate systems are given in order to obtain the simplest possible coordinate system satisfying the matching conditions and boundary conditions for each separate layer. An accessory unknown function is the temperature change over time in the center of symmetry. The use of this function in the heat balance integral method allows for reduction in the solution of the initial partial differential equation to the integration of an ordinary differential equation with respect to the additional unknown function.
Further boundary conditions are defined in such a way that their satisfaction by an unknown solution is equivalent to the satisfaction of the equations at the boundary points. Studies have shown that the equation fulfillment at the boundaries leads to their fulfillment within the regions.</description><identifier>ISSN: 1742-6588</identifier><identifier>EISSN: 1742-6596</identifier><identifier>DOI: 10.1088/1742-6596/1745/1/012073</identifier><language>eng</language><publisher>Bristol: IOP Publishing</publisher><subject>Boundary conditions ; Conduction heating ; Conductive heat transfer ; Coordinates ; Exact solutions ; Heat balance method ; Integrals ; Multilayers ; Ordinary differential equations ; Partial differential equations ; Physics ; Propagation velocity ; Symmetry</subject><ispartof>Journal of physics. Conference series, 2021-02, Vol.1745 (1), p.12073</ispartof><rights>2021. This work is published under http://creativecommons.org/licenses/by/3.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c1953-996cc29d657cc9ae26d75106a5cb46ceb334c66233b29945dd62b2b2a85c395d3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.proquest.com/docview/2512981689?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>314,776,780,25733,27903,27904,36991,44569</link.rule.ids></links><search><creatorcontrib>Trubitsyn, K V</creatorcontrib><creatorcontrib>Mikheeva, G V</creatorcontrib><creatorcontrib>Klebleev, R M</creatorcontrib><creatorcontrib>Kurganova, O Y</creatorcontrib><title>Further boundary conditions in heat conduction problems in multilayer structures</title><title>Journal of physics. Conference series</title><description>This paper presents an approximate analytical solution of the heat conduction problem for a two-layer plate under symmetric boundary conditions of the first kind. The solution was determined on the basis of the property of the parabolic heat transfer equation associated with an infinite velocity of heat propagation, by determining the accessory unknown function and accessory boundary conditions in the integral heat balance method.
Local coordinate systems are given in order to obtain the simplest possible coordinate system satisfying the matching conditions and boundary conditions for each separate layer. An accessory unknown function is the temperature change over time in the center of symmetry. The use of this function in the heat balance integral method allows for reduction in the solution of the initial partial differential equation to the integration of an ordinary differential equation with respect to the additional unknown function.
Further boundary conditions are defined in such a way that their satisfaction by an unknown solution is equivalent to the satisfaction of the equations at the boundary points. Studies have shown that the equation fulfillment at the boundaries leads to their fulfillment within the regions.</description><subject>Boundary conditions</subject><subject>Conduction heating</subject><subject>Conductive heat transfer</subject><subject>Coordinates</subject><subject>Exact solutions</subject><subject>Heat balance method</subject><subject>Integrals</subject><subject>Multilayers</subject><subject>Ordinary differential equations</subject><subject>Partial differential equations</subject><subject>Physics</subject><subject>Propagation velocity</subject><subject>Symmetry</subject><issn>1742-6588</issn><issn>1742-6596</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><recordid>eNo9UMlOwzAQtRBIlMI3EIlziJfYsY-oooBUCQ5wthzbVVMlcfFy6N9jt6gzh3maebM9AB4RfEaQ8wZ1La4ZFawg2qAGIgw7cgUWl8r1BXN-C-5C2ENIsnUL8LVOPu6sr3qXZqP8sdJuNkMc3ByqYa52VsVTKumSqw7e9aOdTrUpjXEY1TF3h-gzIXkb7sHNVo3BPvzHJfhZv36v3uvN59vH6mVTayQoqYVgWmNhGO20FspiZjqKIFNU9y3Ttiek1YxhQnosREuNYbjPrjjVRFBDluDpPDdf9JtsiHLvkp_zSokpwoIjxkVmdWeW9i4Eb7fy4IcpvykRlEU-WYSRRaSCqETyLB_5A9QpY9Q</recordid><startdate>20210201</startdate><enddate>20210201</enddate><creator>Trubitsyn, K V</creator><creator>Mikheeva, G V</creator><creator>Klebleev, R M</creator><creator>Kurganova, O Y</creator><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>H8D</scope><scope>HCIFZ</scope><scope>L7M</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope></search><sort><creationdate>20210201</creationdate><title>Further boundary conditions in heat conduction problems in multilayer structures</title><author>Trubitsyn, K V ; Mikheeva, G V ; Klebleev, R M ; Kurganova, O Y</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1953-996cc29d657cc9ae26d75106a5cb46ceb334c66233b29945dd62b2b2a85c395d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Boundary conditions</topic><topic>Conduction heating</topic><topic>Conductive heat transfer</topic><topic>Coordinates</topic><topic>Exact solutions</topic><topic>Heat balance method</topic><topic>Integrals</topic><topic>Multilayers</topic><topic>Ordinary differential equations</topic><topic>Partial differential equations</topic><topic>Physics</topic><topic>Propagation velocity</topic><topic>Symmetry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Trubitsyn, K V</creatorcontrib><creatorcontrib>Mikheeva, G V</creatorcontrib><creatorcontrib>Klebleev, R M</creatorcontrib><creatorcontrib>Kurganova, O Y</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central</collection><collection>Aerospace Database</collection><collection>SciTech Premium Collection</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><jtitle>Journal of physics. 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The solution was determined on the basis of the property of the parabolic heat transfer equation associated with an infinite velocity of heat propagation, by determining the accessory unknown function and accessory boundary conditions in the integral heat balance method.
Local coordinate systems are given in order to obtain the simplest possible coordinate system satisfying the matching conditions and boundary conditions for each separate layer. An accessory unknown function is the temperature change over time in the center of symmetry. The use of this function in the heat balance integral method allows for reduction in the solution of the initial partial differential equation to the integration of an ordinary differential equation with respect to the additional unknown function.
Further boundary conditions are defined in such a way that their satisfaction by an unknown solution is equivalent to the satisfaction of the equations at the boundary points. Studies have shown that the equation fulfillment at the boundaries leads to their fulfillment within the regions.</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><doi>10.1088/1742-6596/1745/1/012073</doi><oa>free_for_read</oa></addata></record> |
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subjects | Boundary conditions Conduction heating Conductive heat transfer Coordinates Exact solutions Heat balance method Integrals Multilayers Ordinary differential equations Partial differential equations Physics Propagation velocity Symmetry |
title | Further boundary conditions in heat conduction problems in multilayer structures |
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