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Finite deformation analysis of flexoelectric shells
Computer Methods in Applied Mechanics and Engineering, Volume: 447, Start page: 118384
Swansea University Author:
Mokarram Hossain
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Author accepted manuscript document released under the terms of a Creative Commons CC-BY licence using the Swansea University Research Publications Policy (rights retention).
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DOI (Published version): 10.1016/j.cma.2025.118384
Abstract
In this work, a nonlinear shell model for the coupled mechanical and electrical analysis of thinflexoelectric polymers is developed. In addition to the classical terms, contributions from thesecond gradient of deformation, electro-mechanical coupling and flexoelectricity are incorporatedinto the fre...
| Published in: | Computer Methods in Applied Mechanics and Engineering |
|---|---|
| ISSN: | 0045-7825 |
| Published: |
Elsevier BV
2025
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| Online Access: |
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| URI: | https://cronfa.swan.ac.uk/Record/cronfa70379 |
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2025-09-18T07:56:41Z |
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| last_indexed |
2025-10-25T06:47:16Z |
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2025-10-24T15:45:49.3277491 v2 70379 2025-09-18 Finite deformation analysis of flexoelectric shells 140f4aa5c5ec18ec173c8542a7fddafd 0000-0002-4616-1104 Mokarram Hossain Mokarram Hossain true false 2025-09-18 ACEM In this work, a nonlinear shell model for the coupled mechanical and electrical analysis of thinflexoelectric polymers is developed. In addition to the classical terms, contributions from thesecond gradient of deformation, electro-mechanical coupling and flexoelectricity are incorporatedinto the free energy density of these materials. Furthermore, starting from a variationalframework, a nonlinear finite element formulation in the material setting is developed toprovide numerical solutions for various problems. By neglecting the electrical and flexoelectriceffects, the present formulation can reflect the deformation of purely mechanical gradient shells.Conversely, by disregarding the gradient and flexoelectric effects, the present formulation isgreatly capable of modeling the deformation of electro-active shells. The midsurface displacementand director difference vectors are interpolated using 1 shape functions, while 0-continuous interpolation functions are used for the thickness stretching and voltage parameters.Several numerical examples are solved to evaluate performance and robustness of the proposedformulation. The results show that the present formulation yields excellent agreement withthose available in the literature. Moreover, the proposed formulation effectively captures theflexoelectric response of both initially flat and initially curved thin structures experiencing finitedeformations. Journal Article Computer Methods in Applied Mechanics and Engineering 447 118384 Elsevier BV 0045-7825 Flexoelectricity; Shell; Soft dielectric; Finite deformation; Finite element method 1 12 2025 2025-12-01 10.1016/j.cma.2025.118384 COLLEGE NANME Aerospace, Civil, Electrical, and Mechanical Engineering COLLEGE CODE ACEM Swansea University 2025-10-24T15:45:49.3277491 2025-09-18T08:53:53.8270044 Faculty of Science and Engineering School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Mechanical Engineering Farzam Dadgar-Rad 1 Shahab Sahraee 2 Mokarram Hossain 0000-0002-4616-1104 3 Stefan Hartmann 0000-0003-1849-0784 4 70379__35116__5789e0c27110430c81045a38411c2730.pdf 70379.pdf 2025-09-18T08:56:32.4003692 Output 863941 application/pdf Accepted Manuscript true Author accepted manuscript document released under the terms of a Creative Commons CC-BY licence using the Swansea University Research Publications Policy (rights retention). true eng https://creativecommons.org/licenses/by/4.0/deed.en |
| title |
Finite deformation analysis of flexoelectric shells |
| spellingShingle |
Finite deformation analysis of flexoelectric shells Mokarram Hossain |
| title_short |
Finite deformation analysis of flexoelectric shells |
| title_full |
Finite deformation analysis of flexoelectric shells |
| title_fullStr |
Finite deformation analysis of flexoelectric shells |
| title_full_unstemmed |
Finite deformation analysis of flexoelectric shells |
| title_sort |
Finite deformation analysis of flexoelectric shells |
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140f4aa5c5ec18ec173c8542a7fddafd |
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140f4aa5c5ec18ec173c8542a7fddafd_***_Mokarram Hossain |
| author |
Mokarram Hossain |
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Farzam Dadgar-Rad Shahab Sahraee Mokarram Hossain Stefan Hartmann |
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Journal article |
| container_title |
Computer Methods in Applied Mechanics and Engineering |
| container_volume |
447 |
| container_start_page |
118384 |
| publishDate |
2025 |
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Swansea University |
| issn |
0045-7825 |
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10.1016/j.cma.2025.118384 |
| publisher |
Elsevier BV |
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Faculty of Science and Engineering |
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Faculty of Science and Engineering |
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School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Mechanical Engineering{{{_:::_}}}Faculty of Science and Engineering{{{_:::_}}}School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Mechanical Engineering |
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| description |
In this work, a nonlinear shell model for the coupled mechanical and electrical analysis of thinflexoelectric polymers is developed. In addition to the classical terms, contributions from thesecond gradient of deformation, electro-mechanical coupling and flexoelectricity are incorporatedinto the free energy density of these materials. Furthermore, starting from a variationalframework, a nonlinear finite element formulation in the material setting is developed toprovide numerical solutions for various problems. By neglecting the electrical and flexoelectriceffects, the present formulation can reflect the deformation of purely mechanical gradient shells.Conversely, by disregarding the gradient and flexoelectric effects, the present formulation isgreatly capable of modeling the deformation of electro-active shells. The midsurface displacementand director difference vectors are interpolated using 1 shape functions, while 0-continuous interpolation functions are used for the thickness stretching and voltage parameters.Several numerical examples are solved to evaluate performance and robustness of the proposedformulation. The results show that the present formulation yields excellent agreement withthose available in the literature. Moreover, the proposed formulation effectively captures theflexoelectric response of both initially flat and initially curved thin structures experiencing finitedeformations. |
| published_date |
2025-12-01T06:49:29Z |
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1851284174009270272 |
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11.089469 |

