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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$_{3}$...

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Detalles Bibliográficos
Autores principales: Fleiter, Jerome, Ballarino, Amalia, Bonasia, Angelo, Bordini, Bernardo, Richter, David
Lenguaje:eng
Publicado: 2017
Materias:
Acceso en línea:https://dx.doi.org/10.1109/TASC.2017.2672903
http://cds.cern.ch/record/2275318
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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.
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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
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AT ballarinoamalia optimizationofnb3snrutherfordcablesgeometryforthehighluminositylhc
AT bonasiaangelo optimizationofnb3snrutherfordcablesgeometryforthehighluminositylhc
AT bordinibernardo optimizationofnb3snrutherfordcablesgeometryforthehighluminositylhc
AT richterdavid optimizationofnb3snrutherfordcablesgeometryforthehighluminositylhc