Magnetic Design and Code Benchmarking of the SMC (Short Model Coil) Dipole Magnet
Identifieur interne : 000F18 ( Main/Exploration ); précédent : 000F17; suivant : 000F19Magnetic Design and Code Benchmarking of the SMC (Short Model Coil) Dipole Magnet
Auteurs : Pierre Manil [France] ; Federico Regis [Suisse] ; James Rochford [Royaume-Uni] ; Paolo Fessia [Suisse] ; Simon Canfer [Royaume-Uni] ; Elwyn Baynham [Royaume-Uni] ; François Nunio [France] ; Gijs De Rijk [Suisse] ; Pierre Vedrine [France]Source :
- IEEE transactions on applied superconductivity [ 1051-8223 ] ; 2010.
Descripteurs français
- Pascal (Inist)
- Codage, Benchmarking, Dipôle, Aimant accélérateur, Europe, Modèle réduit, CERN, Technique poudre dans tube, Toron, Dégradation, Endommagement, Propriété magnétique, Précontrainte, Champ intense, Modèle 3 dimensions, Modèle non linéaire, Méthode paramétrique, Implémentation, Optimisation, Cale espacement, Electroaimant supraconducteur.
- Wicri :
- topic : Codage.
English descriptors
- KwdEn :
- Accelerator magnets, Benchmarking, CERN, Coding, Damaging, Degradation, Dipole, Europe, High field, Implementation, Magnetic properties, Non linear model, Optimization, Parametric method, Powder in tube technique, Prestress, Scale model, Spacer, Strand, Superconducting magnet, Three dimensional model.
Abstract
The Short Model Coil (SMC) working group was set in February 2007 within the Next European Dipole (NED) program, in order to develop a short-scale model of a Nb3Sn dipole magnet. The SMC group comprises four laboratories: CERN/TE-MSC group (CH), CEA/IRFU (FR), RAL (UK) and LBNL (US). The SMC magnet is designed to reach a peak field of about 13 Tesla (T) on conductor, using a 2500 A/mm2 Powder-In-Tube (PIT) strand. The aim of this magnet device is to study the degradation of the magnetic properties of the Nb3Sn cable, by applying different levels of pre-stress. To fully satisfy this purpose, a versatile and easy-to-assemble structure has been realized. The design of the SMC magnet has been developed from an existing dipole magnet, the SD01, designed, built and tested at LBNL with support from CEA. The goal of the magnetic design presented in this paper is to match the high field region with the high stress region, located along the dipole straight section. For this purpose, three-dimensional nonlinear parametric models have been implemented using three codes (CAST3M, ANSYS, and OPERA). This optimization process has been an opportunity to cross-check the codes. The results of this benchmarking are presented here, along with the final design which incorporates the use of end spacers and a surrounding iron structure to deliver a nominal field of 13 T uniformly distributed along the cable straight section.
Affiliations:
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Le document en format XML
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<series><title level="j" type="main">IEEE transactions on applied superconductivity</title>
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<front><div type="abstract" xml:lang="en">The Short Model Coil (SMC) working group was set in February 2007 within the Next European Dipole (NED) program, in order to develop a short-scale model of a Nb<sub>3</sub>
Sn dipole magnet. The SMC group comprises four laboratories: CERN/TE-MSC group (CH), CEA/IRFU (FR), RAL (UK) and LBNL (US). The SMC magnet is designed to reach a peak field of about 13 Tesla (T) on conductor, using a 2500 A/mm<sup>2</sup>
Powder-In-Tube (PIT) strand. The aim of this magnet device is to study the degradation of the magnetic properties of the Nb<sub>3</sub>
Sn cable, by applying different levels of pre-stress. To fully satisfy this purpose, a versatile and easy-to-assemble structure has been realized. The design of the SMC magnet has been developed from an existing dipole magnet, the SD01, designed, built and tested at LBNL with support from CEA. The goal of the magnetic design presented in this paper is to match the high field region with the high stress region, located along the dipole straight section. For this purpose, three-dimensional nonlinear parametric models have been implemented using three codes (CAST3M, ANSYS, and OPERA). This optimization process has been an opportunity to cross-check the codes. The results of this benchmarking are presented here, along with the final design which incorporates the use of end spacers and a surrounding iron structure to deliver a nominal field of 13 T uniformly distributed along the cable straight section.</div>
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