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A discrete 2-D Formulation for 3-D Field Problems with Continuous Symmetry
We describe a general formalism that allows to reduce the spatial dimension of a field problem from 3-D to (2+1)-D. Subsequently we identify conditions under which the third dimension can be eliminated.We see that the resulting 2-D field problems only decouple if an orthogonality criterion is fulfil...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2010
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1109/TMAG.2010.2045224 http://cds.cern.ch/record/1282387 |
_version_ | 1780920502269771776 |
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author | Auchmann, B Flemisch, B Kurz, S |
author_facet | Auchmann, B Flemisch, B Kurz, S |
author_sort | Auchmann, B |
collection | CERN |
description | We describe a general formalism that allows to reduce the spatial dimension of a field problem from 3-D to (2+1)-D. Subsequently we identify conditions under which the third dimension can be eliminated.We see that the resulting 2-D field problems only decouple if an orthogonality criterion is fulfilled.The approach is based solely on differential-form calculus and can therefore be easily transferred into a discrete setting. As a numerical example we compute the field of twisted wires. |
id | cern-1282387 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2010 |
record_format | invenio |
spelling | cern-12823872019-09-30T06:29:59Zdoi:10.1109/TMAG.2010.2045224http://cds.cern.ch/record/1282387engAuchmann, BFlemisch, BKurz, SA discrete 2-D Formulation for 3-D Field Problems with Continuous SymmetryAccelerators and Storage RingsWe describe a general formalism that allows to reduce the spatial dimension of a field problem from 3-D to (2+1)-D. Subsequently we identify conditions under which the third dimension can be eliminated.We see that the resulting 2-D field problems only decouple if an orthogonality criterion is fulfilled.The approach is based solely on differential-form calculus and can therefore be easily transferred into a discrete setting. As a numerical example we compute the field of twisted wires.CERN-ATS-2010-165oai:cds.cern.ch:12823872010-02-01 |
spellingShingle | Accelerators and Storage Rings Auchmann, B Flemisch, B Kurz, S A discrete 2-D Formulation for 3-D Field Problems with Continuous Symmetry |
title | A discrete 2-D Formulation for 3-D Field Problems with Continuous Symmetry |
title_full | A discrete 2-D Formulation for 3-D Field Problems with Continuous Symmetry |
title_fullStr | A discrete 2-D Formulation for 3-D Field Problems with Continuous Symmetry |
title_full_unstemmed | A discrete 2-D Formulation for 3-D Field Problems with Continuous Symmetry |
title_short | A discrete 2-D Formulation for 3-D Field Problems with Continuous Symmetry |
title_sort | discrete 2-d formulation for 3-d field problems with continuous symmetry |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.1109/TMAG.2010.2045224 http://cds.cern.ch/record/1282387 |
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