3D semi-analytical solution of hygro-thermo-mechanical multilayered doubly-curved shells

Descripción del Articulo

El texto completo de este trabajo no está disponible en el Repositorio Académico UPC por restricciones de la casa editorial donde ha sido publicado.
Detalles Bibliográficos
Autores: Monge, J. C., Mantari, J. L., Arciniega, R. A.
Formato: artículo
Fecha de Publicación:2022
Institución:Universidad Peruana de Ciencias Aplicadas
Repositorio:UPC-Institucional
Lenguaje:inglés
OAI Identifier:oai:repositorioacademico.upc.edu.pe:10757/659241
Enlace del recurso:http://hdl.handle.net/10757/659241
Nivel de acceso:acceso embargado
Materia:Equilibrium equations
Heat conduction
Moisture diffusion Law
Multilayered
Shell
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dc.title.es_PE.fl_str_mv 3D semi-analytical solution of hygro-thermo-mechanical multilayered doubly-curved shells
title 3D semi-analytical solution of hygro-thermo-mechanical multilayered doubly-curved shells
spellingShingle 3D semi-analytical solution of hygro-thermo-mechanical multilayered doubly-curved shells
Monge, J. C.
Equilibrium equations
Heat conduction
Moisture diffusion Law
Multilayered
Shell
title_short 3D semi-analytical solution of hygro-thermo-mechanical multilayered doubly-curved shells
title_full 3D semi-analytical solution of hygro-thermo-mechanical multilayered doubly-curved shells
title_fullStr 3D semi-analytical solution of hygro-thermo-mechanical multilayered doubly-curved shells
title_full_unstemmed 3D semi-analytical solution of hygro-thermo-mechanical multilayered doubly-curved shells
title_sort 3D semi-analytical solution of hygro-thermo-mechanical multilayered doubly-curved shells
author Monge, J. C.
author_facet Monge, J. C.
Mantari, J. L.
Arciniega, R. A.
author_role author
author2 Mantari, J. L.
Arciniega, R. A.
author2_role author
author
dc.contributor.author.fl_str_mv Monge, J. C.
Mantari, J. L.
Arciniega, R. A.
dc.subject.es_PE.fl_str_mv Equilibrium equations
Heat conduction
Moisture diffusion Law
Multilayered
Shell
topic Equilibrium equations
Heat conduction
Moisture diffusion Law
Multilayered
Shell
description El texto completo de este trabajo no está disponible en el Repositorio Académico UPC por restricciones de la casa editorial donde ha sido publicado.
publishDate 2022
dc.date.accessioned.none.fl_str_mv 2022-03-04T13:02:20Z
dc.date.available.none.fl_str_mv 2022-03-04T13:02:20Z
dc.date.issued.fl_str_mv 2022-04-01
dc.type.es_PE.fl_str_mv info:eu-repo/semantics/article
format article
dc.identifier.issn.none.fl_str_mv 01410296
dc.identifier.doi.none.fl_str_mv 10.1016/j.engstruct.2022.113916
dc.identifier.uri.none.fl_str_mv http://hdl.handle.net/10757/659241
dc.identifier.eissn.none.fl_str_mv 18737323
dc.identifier.journal.es_PE.fl_str_mv Engineering Structures
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identifier_str_mv 01410296
10.1016/j.engstruct.2022.113916
18737323
Engineering Structures
2-s2.0-85124429692
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url http://hdl.handle.net/10757/659241
dc.language.iso.es_PE.fl_str_mv eng
language eng
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dc.publisher.es_PE.fl_str_mv Elsevier Ltd
dc.source.none.fl_str_mv reponame:UPC-Institucional
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dc.source.journaltitle.none.fl_str_mv Engineering Structures
dc.source.volume.none.fl_str_mv 256
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spelling 1ab4da19501604b4a66fb77f554d6d8f500ce793fbc9dfb602a7033119b1c5382543be5aa610b96c77740439e04827deb9eMonge, J. C.Mantari, J. L.Arciniega, R. A.2022-03-04T13:02:20Z2022-03-04T13:02:20Z2022-04-010141029610.1016/j.engstruct.2022.113916http://hdl.handle.net/10757/65924118737323Engineering Structures2-s2.0-85124429692SCOPUS_ID:85124429692S01410296220007480000 0001 2196 144XEl texto completo de este trabajo no está disponible en el Repositorio Académico UPC por restricciones de la casa editorial donde ha sido publicado.In this paper, a three-dimensional bending solution of doubly-curved shells subjected to mechanical, thermal and hygrothermal load is studied. Through-the-thickness temperature of the shell is modeled by Fourier's heat conduction equation. Fick's moisture diffusion law equation is used to determine the hygro-thermal profile through-the-thickness. The partial differential equations are solved by using the Navier closed form summations which are valid only for shells with constant radii of curvature among the midsurface and with simply supported boundary conditions on its shell's edges. The shell governing equations are solved by discretizing the thickness profile via Legendre's grid distribution and by using the Differential Quadrature Method (DQM). The Layerwise capabilities of the method is guaranteed by imposing the inter-laminar continuity of out-of-the-plane stresses, displacements, temperature and hygrothermal load thickness profile. The zero-stress condition for the transverse shear stresses is imposed due to the fact that no mechanical loads are applied in those directions. Results for cylindrical, spherical panels and rectangular plates are presented. Comparisons are made with Layerwise and three-dimensional solutions available in literature. The results have strong accuracy and a benchmark problem is delivered.Consejo Nacional de Ciencia, Tecnología e Innovación Tecnológicaapplication/htmlengElsevier Ltdhttps://www.sciencedirect.com/science/article/abs/pii/S0141029622000748info:eu-repo/semantics/embargoedAccessAttribution-NonCommercial-ShareAlike 4.0 Internationalhttp://creativecommons.org/licenses/by-nc-sa/4.0/Equilibrium equationsHeat conductionMoisture diffusion LawMultilayeredShell3D semi-analytical solution of hygro-thermo-mechanical multilayered doubly-curved shellsinfo:eu-repo/semantics/articleEngineering Structures256reponame:UPC-Institucionalinstname:Universidad Peruana de Ciencias Aplicadasinstacron:UPCLICENSElicense.txtlicense.txttext/plain; charset=utf-81748https://repositorioacademico.upc.edu.pe/bitstream/10757/659241/2/license.txt8a4605be74aa9ea9d79846c1fba20a33MD52falseCC-LICENSElicense_rdflicense_rdfapplication/rdf+xml; charset=utf-81031https://repositorioacademico.upc.edu.pe/bitstream/10757/659241/1/license_rdf934f4ca17e109e0a05eaeaba504d7ce4MD51false10757/659241oai:repositorioacademico.upc.edu.pe:10757/6592412022-03-04 13:04:50.643Repositorio académico upcupc@openrepository.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