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$J_{C}(B,T,\epsilon)$ Parameterization for the ITER Nb$_{3}$Sn Production
A number of models for the critical surface of Nb$_{3}$Sn, and in general A15 superconductors, have been developed in the past years. This paper compares the most common parameterizations using consistent notation. Although the parameterizations appear dissimilar at first sight, they are in reality...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
2009
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Acceso en línea: | https://dx.doi.org/10.1109/TASC.2009.2018278 http://cds.cern.ch/record/1192836 |
_version_ | 1780916709248466944 |
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author | Bottura, L Bordini, B |
author_facet | Bottura, L Bordini, B |
author_sort | Bottura, L |
collection | CERN |
description | A number of models for the critical surface of Nb$_{3}$Sn, and in general A15 superconductors, have been developed in the past years. This paper compares the most common parameterizations using consistent notation. Although the parameterizations appear dissimilar at first sight, they are in reality all based on a fit of the normalised pinning force vs. the reduced field, and have similar scalings for the critical field and critical temperature based on a Unified Scaling Law. In this paper we take the various parameterizations as a basis for a generic scaling proposed for the characterization and production follow-up of the ITER Nb$_{3}$Sn strands. The accuracy of the scaling is estimated using the fitting residuals on various sets of Ic(B,T,e) data available in literature. We discuss the results, and give our view of the work towards a unified, practical parameterization. |
id | cern-1192836 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2009 |
record_format | invenio |
spelling | cern-11928362019-09-30T06:29:59Zdoi:10.1109/TASC.2009.2018278http://cds.cern.ch/record/1192836engBottura, LBordini, B$J_{C}(B,T,\epsilon)$ Parameterization for the ITER Nb$_{3}$Sn ProductionAccelerators and Storage RingsEngineeringA number of models for the critical surface of Nb$_{3}$Sn, and in general A15 superconductors, have been developed in the past years. This paper compares the most common parameterizations using consistent notation. Although the parameterizations appear dissimilar at first sight, they are in reality all based on a fit of the normalised pinning force vs. the reduced field, and have similar scalings for the critical field and critical temperature based on a Unified Scaling Law. In this paper we take the various parameterizations as a basis for a generic scaling proposed for the characterization and production follow-up of the ITER Nb$_{3}$Sn strands. The accuracy of the scaling is estimated using the fitting residuals on various sets of Ic(B,T,e) data available in literature. We discuss the results, and give our view of the work towards a unified, practical parameterization.CERN-AT-2008-036oai:cds.cern.ch:11928362009-03-01 |
spellingShingle | Accelerators and Storage Rings Engineering Bottura, L Bordini, B $J_{C}(B,T,\epsilon)$ Parameterization for the ITER Nb$_{3}$Sn Production |
title | $J_{C}(B,T,\epsilon)$ Parameterization for the ITER Nb$_{3}$Sn Production |
title_full | $J_{C}(B,T,\epsilon)$ Parameterization for the ITER Nb$_{3}$Sn Production |
title_fullStr | $J_{C}(B,T,\epsilon)$ Parameterization for the ITER Nb$_{3}$Sn Production |
title_full_unstemmed | $J_{C}(B,T,\epsilon)$ Parameterization for the ITER Nb$_{3}$Sn Production |
title_short | $J_{C}(B,T,\epsilon)$ Parameterization for the ITER Nb$_{3}$Sn Production |
title_sort | $j_{c}(b,t,\epsilon)$ parameterization for the iter nb$_{3}$sn production |
topic | Accelerators and Storage Rings Engineering |
url | https://dx.doi.org/10.1109/TASC.2009.2018278 http://cds.cern.ch/record/1192836 |
work_keys_str_mv | AT bottural jcbtepsilonparameterizationfortheiternb3snproduction AT bordinib jcbtepsilonparameterizationfortheiternb3snproduction |