Thermal bending response of functionally graded magneto-electric–elastic shell employing non-polynomial model
Descripción del Articulo
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...
| Autores: | , |
|---|---|
| Formato: | artículo |
| Fecha de Publicación: | 2022 |
| Institución: | Universidad Nacional de Ingeniería |
| Repositorio: | UNI-Tesis |
| Lenguaje: | inglés |
| OAI Identifier: | oai:cybertesis.uni.edu.pe:20.500.14076/29119 |
| Enlace del recurso: | http://hdl.handle.net/20.500.14076/29119 https://doi.org/10.1080/15376494.2022.2064570 |
| Nivel de acceso: | acceso abierto |
| Materia: | 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 Monge, J.C. 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. |
| author |
Monge, J.C. |
| author_facet |
Monge, J.C. Mantari, J.L. |
| author_role |
author |
| author2 |
Mantari, J.L. |
| author2_role |
author |
| dc.contributor.author.fl_str_mv |
Monge, J.C. Mantari, J.L. |
| 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 |
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info:eu-repo/semantics/article |
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http://purl.org/coar/version/c_970fb48d4fbd8a85 |
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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 |
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eng |
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CrossMark |
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info:eu-repo/semantics/openAccess |
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http://creativecommons.org/licenses/by-nc-nd/4.0/ |
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openAccess |
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http://creativecommons.org/licenses/by-nc-nd/4.0/ |
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application/pdf |
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Taylor & Francis |
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Universidad Nacional de Ingeniería Repositorio Institucional - UNI |
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Monge, J.C.Mantari, J.L.Mantari, J.L.Monge, J.C.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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 |
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La información contenida en este registro es de entera responsabilidad de la institución que gestiona el repositorio institucional donde esta contenido este documento o set de datos. El CONCYTEC no se hace responsable por los contenidos (publicaciones y/o datos) accesibles a través del Repositorio Nacional Digital de Ciencia, Tecnología e Innovación de Acceso Abierto (ALICIA).