Modeling the Converse Magnetoelectric Effect in the Low-Frequency Range
This article is devoted to the theory of the converse magnetoelectric (CME) effect for the longitudinal, bending, longitudinal-shear, and torsional resonance modes and its quasi-static regime. In contrast to the direct ME effect (DME), these issues have not been studied in sufficient detail in the l...
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| Format: | Article |
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MDPI AG
2023-12-01
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| Series: | Sensors |
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| Online Access: | https://www.mdpi.com/1424-8220/24/1/151 |
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| author | Mirza Bichurin Oleg Sokolov Sergey Ivanov Viktor Leontiev Vyacheslav Lobekin Gennady Semenov Yaojin Wang |
| author_facet | Mirza Bichurin Oleg Sokolov Sergey Ivanov Viktor Leontiev Vyacheslav Lobekin Gennady Semenov Yaojin Wang |
| author_sort | Mirza Bichurin |
| collection | DOAJ |
| description | This article is devoted to the theory of the converse magnetoelectric (CME) effect for the longitudinal, bending, longitudinal-shear, and torsional resonance modes and its quasi-static regime. In contrast to the direct ME effect (DME), these issues have not been studied in sufficient detail in the literature. However, in a number of cases, in particular in the study of low-frequency ME antennas, the results obtained are of interest. Detailed calculations with examples were carried out for the longitudinal mode on the symmetric and asymmetric structures based on Metglas/PZT (LN); the bending mode was considered for the asymmetric free structure and structure with rigidly fixed left-end Metglas/PZT (LN); the longitudinal-shear and torsional modes were investigated for the symmetric and asymmetric free structures based on Metglas/GaAs. For the identification of the torsion mode, it was suggested to perform an experiment on the ME structure based on Metglas/bimorphic LN. All calculation results are presented in the form of graphs for the CME coefficients. |
| first_indexed | 2024-03-08T14:57:08Z |
| format | Article |
| id | doaj.art-3d05c2b3c4f34378abe87aa8866dd9fb |
| institution | Directory Open Access Journal |
| issn | 1424-8220 |
| language | English |
| last_indexed | 2024-03-08T14:57:08Z |
| publishDate | 2023-12-01 |
| publisher | MDPI AG |
| record_format | Article |
| series | Sensors |
| spelling | doaj.art-3d05c2b3c4f34378abe87aa8866dd9fb2024-01-10T15:08:47ZengMDPI AGSensors1424-82202023-12-0124115110.3390/s24010151Modeling the Converse Magnetoelectric Effect in the Low-Frequency RangeMirza Bichurin0Oleg Sokolov1Sergey Ivanov2Viktor Leontiev3Vyacheslav Lobekin4Gennady Semenov5Yaojin Wang6Yaroslav-the-Wise Novgorod State University, 173003 Velikiy Novgorod, RussiaYaroslav-the-Wise Novgorod State University, 173003 Velikiy Novgorod, RussiaYaroslav-the-Wise Novgorod State University, 173003 Velikiy Novgorod, RussiaYaroslav-the-Wise Novgorod State University, 173003 Velikiy Novgorod, RussiaYaroslav-the-Wise Novgorod State University, 173003 Velikiy Novgorod, RussiaYaroslav-the-Wise Novgorod State University, 173003 Velikiy Novgorod, RussiaSchool of Materials Science and Engineering, Nanjing University of Science and Technology, Nanjing 210094, ChinaThis article is devoted to the theory of the converse magnetoelectric (CME) effect for the longitudinal, bending, longitudinal-shear, and torsional resonance modes and its quasi-static regime. In contrast to the direct ME effect (DME), these issues have not been studied in sufficient detail in the literature. However, in a number of cases, in particular in the study of low-frequency ME antennas, the results obtained are of interest. Detailed calculations with examples were carried out for the longitudinal mode on the symmetric and asymmetric structures based on Metglas/PZT (LN); the bending mode was considered for the asymmetric free structure and structure with rigidly fixed left-end Metglas/PZT (LN); the longitudinal-shear and torsional modes were investigated for the symmetric and asymmetric free structures based on Metglas/GaAs. For the identification of the torsion mode, it was suggested to perform an experiment on the ME structure based on Metglas/bimorphic LN. All calculation results are presented in the form of graphs for the CME coefficients.https://www.mdpi.com/1424-8220/24/1/151magnetoelectric effectdirect magnetoelectric effectconverse magnetoelectric effectmagnetoelectric compositemagnetoelectric coefficientelectromechanical resonance |
| spellingShingle | Mirza Bichurin Oleg Sokolov Sergey Ivanov Viktor Leontiev Vyacheslav Lobekin Gennady Semenov Yaojin Wang Modeling the Converse Magnetoelectric Effect in the Low-Frequency Range Sensors magnetoelectric effect direct magnetoelectric effect converse magnetoelectric effect magnetoelectric composite magnetoelectric coefficient electromechanical resonance |
| title | Modeling the Converse Magnetoelectric Effect in the Low-Frequency Range |
| title_full | Modeling the Converse Magnetoelectric Effect in the Low-Frequency Range |
| title_fullStr | Modeling the Converse Magnetoelectric Effect in the Low-Frequency Range |
| title_full_unstemmed | Modeling the Converse Magnetoelectric Effect in the Low-Frequency Range |
| title_short | Modeling the Converse Magnetoelectric Effect in the Low-Frequency Range |
| title_sort | modeling the converse magnetoelectric effect in the low frequency range |
| topic | magnetoelectric effect direct magnetoelectric effect converse magnetoelectric effect magnetoelectric composite magnetoelectric coefficient electromechanical resonance |
| url | https://www.mdpi.com/1424-8220/24/1/151 |
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