A Three-Dimensional Electromagnetic Shell Finite Element for Coupled Vector-Scalar Potential Formulations
Identifieur interne :
001311 ( PascalFrancis/Corpus );
précédent :
001310;
suivant :
001312
A Three-Dimensional Electromagnetic Shell Finite Element for Coupled Vector-Scalar Potential Formulations
Auteurs : P. Thomas ;
Y. Le MenachSource :
-
IEEE transactions on magnetics [ 0018-9464 ] ; 2012.
RBID : Pascal:12-0241374
Descripteurs français
English descriptors
Abstract
In many eddy current problems solved by FEM, meshing of the skin depth leads to CAD difficulties and large computing. In order to avoid such problems, one currently use surface impedance conditions: boundary conditions in the case of massive conductors or transmission conditions or shell elements in the case of thin conducting layers. In this paper, we propose a new shell finite element with arbitrary thickness that is compatible with the (A -
) and (T - Ω) formulations. Both formulations exist in some general purpose finite element electromagnetic codes like Code_Carmel3D. To validate the approach, two elementary numerical tests are treated.
Notice en format standard (ISO 2709)
Pour connaître la documentation sur le format Inist Standard.
| pA |
| A01 | 01 | 1 | | @0 0018-9464 |
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| A02 | 01 | | | @0 IEMGAQ |
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| A03 | | 1 | | @0 IEEE trans. magn. |
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| A05 | | | | @2 48 |
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| A06 | | | | @2 2 |
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| A08 | 01 | 1 | ENG | @1 A Three-Dimensional Electromagnetic Shell Finite Element for Coupled Vector-Scalar Potential Formulations |
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| A09 | 01 | 1 | ENG | @1 COMPUMAG 2011: Selected papers from the 18th International Conference on the Computation of Electromagnetic Fields, Sydney, Australia, July 12-15, 2011 |
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| A11 | 01 | 1 | | @1 THOMAS (P.) |
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| A11 | 02 | 1 | | @1 LE MENACH (Y.) |
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| A12 | 01 | 1 | | @1 TAKAHASHI (Norio) @9 ed. |
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| A12 | 02 | 1 | | @1 DORRELL (David) @9 ed. |
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| A12 | 03 | 1 | | @1 GUO (Youguang) @9 ed. |
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| A14 | 01 | | | @1 Laboratoire d'Analyse des Materiels Electriques, Electricité de France 92141 @2 Clamart @3 FRA @Z 1 aut. @Z 2 aut. |
|---|
| A14 | 02 | | | @1 Université Lillel, L2EP @2 59655 Villeneuve d'Ascq @3 FRA @Z 1 aut. @Z 2 aut. |
|---|
| A15 | 01 | | | @1 Okayama University @2 Okayama @3 JPN @Z 1 aut. |
|---|
| A15 | 02 | | | @1 University of Technology @2 Sydney @3 AUS @Z 2 aut. @Z 3 aut. |
|---|
| A18 | 01 | 1 | | @1 International Compumag Society @3 INT @9 org-cong. |
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| A20 | | | | @1 823-826 |
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| A21 | | | | @1 2012 |
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| A23 | 01 | | | @0 ENG |
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| A43 | 01 | | | @1 INIST @2 222H6 @5 354000506946041630 |
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| A44 | | | | @0 0000 @1 © 2012 INIST-CNRS. All rights reserved. |
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| A45 | | | | @0 7 ref. |
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| A47 | 01 | 1 | | @0 12-0241374 |
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| A60 | | | | @1 P @2 C |
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| A61 | | | | @0 A |
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| A64 | 01 | 1 | | @0 IEEE transactions on magnetics |
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| A66 | 01 | | | @0 USA |
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| C01 | 01 | | ENG | @0 In many eddy current problems solved by FEM, meshing of the skin depth leads to CAD difficulties and large computing. In order to avoid such problems, one currently use surface impedance conditions: boundary conditions in the case of massive conductors or transmission conditions or shell elements in the case of thin conducting layers. In this paper, we propose a new shell finite element with arbitrary thickness that is compatible with the (A - <phi>) and (T - Ω) formulations. Both formulations exist in some general purpose finite element electromagnetic codes like Code_Carmel3D. To validate the approach, two elementary numerical tests are treated. |
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| C02 | 01 | 3 | | @0 001B80A90 |
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| C03 | 01 | 3 | FRE | @0 Méthode élément fini @5 55 |
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| C03 | 01 | 3 | ENG | @0 Finite element method @5 55 |
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| C03 | 02 | 3 | FRE | @0 Modélisation @5 56 |
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| C03 | 02 | 3 | ENG | @0 Modelling @5 56 |
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| C03 | 03 | 3 | FRE | @0 Potentiel @5 57 |
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| C03 | 03 | 3 | ENG | @0 Potentials @5 57 |
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| C03 | 04 | 3 | FRE | @0 Courant Foucault @5 58 |
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| C03 | 04 | 3 | ENG | @0 Eddy currents @5 58 |
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| C03 | 05 | 3 | FRE | @0 Champ électromagnétique @5 59 |
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| C03 | 05 | 3 | ENG | @0 Electromagnetic fields @5 59 |
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| C03 | 06 | 3 | FRE | @0 Propriété magnétique @5 60 |
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| C03 | 06 | 3 | ENG | @0 Magnetic properties @5 60 |
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| N21 | | | | @1 184 |
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| N44 | 01 | | | @1 OTO |
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| N82 | | | | @1 OTO |
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| pR |
| A30 | 01 | 1 | ENG | @1 COMPUMAG 2011 International Conference on the Computation of Electromagnetic Fields @2 18 @3 Sydney AUS @4 2011-07-12 |
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Format Inist (serveur)
| NO : | PASCAL 12-0241374 INIST |
|---|
| ET : | A Three-Dimensional Electromagnetic Shell Finite Element for Coupled Vector-Scalar Potential Formulations |
|---|
| AU : | THOMAS (P.); LE MENACH (Y.); TAKAHASHI (Norio); DORRELL (David); GUO (Youguang) |
|---|
| AF : | Laboratoire d'Analyse des Materiels Electriques, Electricité de France 92141/Clamart/France (1 aut., 2 aut.); Université Lillel, L2EP/59655 Villeneuve d'Ascq/France (1 aut., 2 aut.); Okayama University/Okayama/Japon (1 aut.); University of Technology/Sydney/Australie (2 aut., 3 aut.) |
|---|
| DT : | Publication en série; Congrès; Niveau analytique |
|---|
| SO : | IEEE transactions on magnetics; ISSN 0018-9464; Coden IEMGAQ; Etats-Unis; Da. 2012; Vol. 48; No. 2; Pp. 823-826; Bibl. 7 ref. |
|---|
| LA : | Anglais |
|---|
| EA : | In many eddy current problems solved by FEM, meshing of the skin depth leads to CAD difficulties and large computing. In order to avoid such problems, one currently use surface impedance conditions: boundary conditions in the case of massive conductors or transmission conditions or shell elements in the case of thin conducting layers. In this paper, we propose a new shell finite element with arbitrary thickness that is compatible with the (A - <phi>) and (T - Ω) formulations. Both formulations exist in some general purpose finite element electromagnetic codes like Code_Carmel3D. To validate the approach, two elementary numerical tests are treated. |
|---|
| CC : | 001B80A90 |
|---|
| FD : | Méthode élément fini; Modélisation; Potentiel; Courant Foucault; Champ électromagnétique; Propriété magnétique |
|---|
| ED : | Finite element method; Modelling; Potentials; Eddy currents; Electromagnetic fields; Magnetic properties |
|---|
| LO : | INIST-222H6.354000506946041630 |
|---|
| ID : | 12-0241374 |
|---|
Links to Exploration step
Pascal:12-0241374
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<ET>A Three-Dimensional Electromagnetic Shell Finite Element for Coupled Vector-Scalar Potential Formulations</ET>
<AU>THOMAS (P.); LE MENACH (Y.); TAKAHASHI (Norio); DORRELL (David); GUO (Youguang)</AU>
<AF>Laboratoire d'Analyse des Materiels Electriques, Electricité de France 92141/Clamart/France (1 aut., 2 aut.); Université Lillel, L2EP/59655 Villeneuve d'Ascq/France (1 aut., 2 aut.); Okayama University/Okayama/Japon (1 aut.); University of Technology/Sydney/Australie (2 aut., 3 aut.)</AF>
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