Thermal bending response of functionally graded magneto-electric–elastic shell employing non-polynomial model

The present mathematical model for complex shells is given in the framework of Carrera unified formulation. The mechanical, electrical, and magnetic equations are derived in terms of the principle of virtual displacement, Maxwell’s equations and Gauss equations. Fourier’s heat conduction equation is...

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Detalles Bibliográficos
Autores: Mantari, J.L., Monge, J.C.
Tipo de recurso: artículo
Fecha de publicación:2022
País:Perú
Institución:Universidad Nacional de Ingeniería
Repositorio:UNI-Tesis
Idioma:inglés
OAI Identifier:oai:cybertesis.uni.edu.pe:20.500.14076/29119
Acceso en línea:http://hdl.handle.net/20.500.14076/29119
https://doi.org/10.1080/15376494.2022.2064570
Access Level:acceso abierto
Palabra clave:Magneto-electro–elastic material
Functionally graded material
Shell
Carrera’s unified formulation
Differential quadrature
Heat conduction
https://purl.org/pe-repo/ocde/ford#1.03.03
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dc.title.en.fl_str_mv Thermal bending response of functionally graded magneto-electric–elastic shell employing non-polynomial model
title Thermal bending response of functionally graded magneto-electric–elastic shell employing non-polynomial model
spellingShingle Thermal bending response of functionally graded magneto-electric–elastic shell employing non-polynomial model
Mantari, J.L.
Magneto-electro–elastic material
Functionally graded material
Shell
Carrera’s unified formulation
Differential quadrature
Heat conduction
https://purl.org/pe-repo/ocde/ford#1.03.03
title_short Thermal bending response of functionally graded magneto-electric–elastic shell employing non-polynomial model
title_full Thermal bending response of functionally graded magneto-electric–elastic shell employing non-polynomial model
title_fullStr Thermal bending response of functionally graded magneto-electric–elastic shell employing non-polynomial model
title_full_unstemmed Thermal bending response of functionally graded magneto-electric–elastic shell employing non-polynomial model
title_sort Thermal bending response of functionally graded magneto-electric–elastic shell employing non-polynomial model
dc.creator.none.fl_str_mv Mantari, J.L.
Monge, J.C.
Monge, J.C.
Mantari, J.L.
author Mantari, J.L.
author_facet Mantari, J.L.
Monge, J.C.
author_role author
author2 Monge, J.C.
author2_role author
dc.subject.en.fl_str_mv Magneto-electro–elastic material
Functionally graded material
Shell
Carrera’s unified formulation
Differential quadrature
Heat conduction
topic Magneto-electro–elastic material
Functionally graded material
Shell
Carrera’s unified formulation
Differential quadrature
Heat conduction
https://purl.org/pe-repo/ocde/ford#1.03.03
dc.subject.ocde.es.fl_str_mv https://purl.org/pe-repo/ocde/ford#1.03.03
description The present mathematical model for complex shells is given in the framework of Carrera unified formulation. The mechanical, electrical, and magnetic equations are derived in terms of the principle of virtual displacement, Maxwell’s equations and Gauss equations. Fourier’s heat conduction equation is used. The governing equations are discretized by the Chebyshev–Gauss–Lobatto and solved with the differential quadrature method. The three-dimensional (3D) equilibrium for mechanical, electrical, and magnetic equations are employed for recovering the transverse stresses, electrical displacement and magnetic induction. Finally, quasi-3D solutions for cycloidal shell of revolution and a funnel panel are introduced in this paper.
publishDate 2022
dc.date.accessioned.none.fl_str_mv 2026-03-30T20:44:34Z
dc.date.available.none.fl_str_mv 2026-03-30T20:44:34Z
dc.date.issued.fl_str_mv 2022-05
dc.type.es.fl_str_mv info:eu-repo/semantics/article
dc.type.version.es.fl_str_mv http://purl.org/coar/version/c_970fb48d4fbd8a85
format article
dc.identifier.uri.none.fl_str_mv http://hdl.handle.net/20.500.14076/29119
dc.identifier.doi.es.fl_str_mv https://doi.org/10.1080/15376494.2022.2064570
url http://hdl.handle.net/20.500.14076/29119
https://doi.org/10.1080/15376494.2022.2064570
dc.language.iso.en.fl_str_mv eng
language eng
dc.relation.ispartof.es.fl_str_mv CrossMark
dc.rights.es.fl_str_mv info:eu-repo/semantics/openAccess
dc.rights.uri.es.fl_str_mv http://creativecommons.org/licenses/by-nc-nd/4.0/
eu_rights_str_mv openAccess
rights_invalid_str_mv http://creativecommons.org/licenses/by-nc-nd/4.0/
dc.format.es.fl_str_mv application/pdf
dc.publisher.es.fl_str_mv Taylor & Francis
dc.source.es.fl_str_mv Universidad Nacional de Ingeniería
Repositorio Institucional - UNI
dc.source.none.fl_str_mv reponame:UNI-Tesis
instname:Universidad Nacional de Ingeniería
instacron:UNI
instname_str Universidad Nacional de Ingeniería
instacron_str UNI
institution UNI
reponame_str UNI-Tesis
collection UNI-Tesis
bitstream.url.fl_str_mv http://cybertesis.uni.edu.pe/bitstream/20.500.14076/29119/2/license.txt
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spelling Mantari, J.L.Monge, J.C.Monge, J.C.Mantari, J.L.2026-03-30T20:44:34Z2026-03-30T20:44:34Z2022-05http://hdl.handle.net/20.500.14076/29119https://doi.org/10.1080/15376494.2022.2064570The present mathematical model for complex shells is given in the framework of Carrera unified formulation. The mechanical, electrical, and magnetic equations are derived in terms of the principle of virtual displacement, Maxwell’s equations and Gauss equations. Fourier’s heat conduction equation is used. The governing equations are discretized by the Chebyshev–Gauss–Lobatto and solved with the differential quadrature method. The three-dimensional (3D) equilibrium for mechanical, electrical, and magnetic equations are employed for recovering the transverse stresses, electrical displacement and magnetic induction. Finally, quasi-3D solutions for cycloidal shell of revolution and a funnel panel are introduced in this paper.Submitted by Quispe Rabanal Flavio (flaviofime@hotmail.com) on 2026-03-30T20:44:34Z No. of bitstreams: 1 monge_j.pdf: 3208519 bytes, checksum: c59bb6763586904fa1712ad145bba3ae (MD5)Made available in DSpace on 2026-03-30T20:44:34Z (GMT). No. of bitstreams: 1 monge_j.pdf: 3208519 bytes, checksum: c59bb6763586904fa1712ad145bba3ae (MD5) Previous issue date: 2022-05Este trabajo fue financiado por el Fondo Nacional de Desarrollo Científico, Tecnológico y de Innovación Tecnológica (Fondecyt - Perú) en el marco del "Desarrollo de materiales avanzados para el diseño de nuevos productos y servicios tecnológicos para la minería Peruana" [número de contrato 032-2019]application/pdfengTaylor & FrancisCrossMarkinfo:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-nd/4.0/Universidad Nacional de IngenieríaRepositorio Institucional - UNIreponame:UNI-Tesisinstname:Universidad Nacional de Ingenieríainstacron:UNIMagneto-electro–elastic materialFunctionally graded materialShellCarrera’s unified formulationDifferential quadratureHeat conductionhttps://purl.org/pe-repo/ocde/ford#1.03.03Thermal bending response of functionally graded magneto-electric–elastic shell employing non-polynomial modelinfo:eu-repo/semantics/articlehttp://purl.org/coar/version/c_970fb48d4fbd8a85LICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://cybertesis.uni.edu.pe/bitstream/20.500.14076/29119/2/license.txt8a4605be74aa9ea9d79846c1fba20a33MD5220.500.14076/29119oai:cybertesis.uni.edu.pe:20.500.14076/291192026-03-30 15:52:20.589Repositorio Institucional Universidad Nacional de Ingenieríarepositorio@uni.edu.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