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Optimization of Nb$_{3}$Sn Rutherford Cables Geometry for the High Luminosity LHC
The quadrupole and dipole magnets for the LHC High Luminosity (HL-LHC) upgrade will be based on Nb$_{3}$Sn Rutherford cables that operate at 1.9 K and experience magnetic fields of up to about 12 T. An important step in the design of these magnets is the development of the high aspect ratio Nb$_{3}$...
Autores principales: | , , , , |
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Lenguaje: | eng |
Publicado: |
2017
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1109/TASC.2017.2672903 http://cds.cern.ch/record/2275318 |
_version_ | 1780955155026411520 |
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author | Fleiter, Jerome Ballarino, Amalia Bonasia, Angelo Bordini, Bernardo Richter, David |
author_facet | Fleiter, Jerome Ballarino, Amalia Bonasia, Angelo Bordini, Bernardo Richter, David |
author_sort | Fleiter, Jerome |
collection | CERN |
description | The quadrupole and dipole magnets for the LHC High Luminosity (HL-LHC) upgrade will be based on Nb$_{3}$Sn Rutherford cables that operate at 1.9 K and experience magnetic fields of up to about 12 T. An important step in the design of these magnets is the development of the high aspect ratio Nb$_{3}$Sn cables to achieve the nominal field with sufficient margin. The strong plastic deformation of unreacted $Nb_3Sn$ strands during the Rutherford cabling process may induce non negligible $I_c$ and RRR degradation. In this paper, the cabling degradation is investigated as a function of the cable geometry for both PIT and RRP conductors. Based on this analysis, new baseline geometries for both 11 T and QXF magnets of HL-LHC are proposed. |
id | oai-inspirehep.net-1518312 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2017 |
record_format | invenio |
spelling | oai-inspirehep.net-15183122019-09-30T06:29:59Zdoi:10.1109/TASC.2017.2672903http://cds.cern.ch/record/2275318engFleiter, JeromeBallarino, AmaliaBonasia, AngeloBordini, BernardoRichter, DavidOptimization of Nb$_{3}$Sn Rutherford Cables Geometry for the High Luminosity LHCDetectors and Experimental TechniquesDetectors and Experimental TechniquesAccelerators and Storage RingsThe quadrupole and dipole magnets for the LHC High Luminosity (HL-LHC) upgrade will be based on Nb$_{3}$Sn Rutherford cables that operate at 1.9 K and experience magnetic fields of up to about 12 T. An important step in the design of these magnets is the development of the high aspect ratio Nb$_{3}$Sn cables to achieve the nominal field with sufficient margin. The strong plastic deformation of unreacted $Nb_3Sn$ strands during the Rutherford cabling process may induce non negligible $I_c$ and RRR degradation. In this paper, the cabling degradation is investigated as a function of the cable geometry for both PIT and RRP conductors. Based on this analysis, new baseline geometries for both 11 T and QXF magnets of HL-LHC are proposed.oai:inspirehep.net:15183122017 |
spellingShingle | Detectors and Experimental Techniques Detectors and Experimental Techniques Accelerators and Storage Rings Fleiter, Jerome Ballarino, Amalia Bonasia, Angelo Bordini, Bernardo Richter, David Optimization of Nb$_{3}$Sn Rutherford Cables Geometry for the High Luminosity LHC |
title | Optimization of Nb$_{3}$Sn Rutherford Cables Geometry for the High Luminosity LHC |
title_full | Optimization of Nb$_{3}$Sn Rutherford Cables Geometry for the High Luminosity LHC |
title_fullStr | Optimization of Nb$_{3}$Sn Rutherford Cables Geometry for the High Luminosity LHC |
title_full_unstemmed | Optimization of Nb$_{3}$Sn Rutherford Cables Geometry for the High Luminosity LHC |
title_short | Optimization of Nb$_{3}$Sn Rutherford Cables Geometry for the High Luminosity LHC |
title_sort | optimization of nb$_{3}$sn rutherford cables geometry for the high luminosity lhc |
topic | Detectors and Experimental Techniques Detectors and Experimental Techniques Accelerators and Storage Rings |
url | https://dx.doi.org/10.1109/TASC.2017.2672903 http://cds.cern.ch/record/2275318 |
work_keys_str_mv | AT fleiterjerome optimizationofnb3snrutherfordcablesgeometryforthehighluminositylhc AT ballarinoamalia optimizationofnb3snrutherfordcablesgeometryforthehighluminositylhc AT bonasiaangelo optimizationofnb3snrutherfordcablesgeometryforthehighluminositylhc AT bordinibernardo optimizationofnb3snrutherfordcablesgeometryforthehighluminositylhc AT richterdavid optimizationofnb3snrutherfordcablesgeometryforthehighluminositylhc |