Cargando…
Quench propagation in Nb$_{3}$Sn cos-theta 11 T dipole model magnets in high stress areas
A large number of training quenches at various currents, temperatures, and ramp rates, have been performed on six 11 T dipole model magnets. Quenches in the midplane of these magnets were of special interest, since the quench current in the last three models measured in 2016 was limited to between 8...
Autores principales: | , , , , , , , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2018
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1109/TASC.2018.2818282 http://cds.cern.ch/record/2674333 |
_version_ | 1780962618147602432 |
---|---|
author | Mangiarotti, Franco J Willering, Gerard P Bajas, Hugues Bajko, Marta Bordini, Bernardo Bottura, Luca Izquierdo Bermudez, Susana Löffler, Christian H Gomez, Jose V Lorenzo Savary, Frederic Probst, Matthias |
author_facet | Mangiarotti, Franco J Willering, Gerard P Bajas, Hugues Bajko, Marta Bordini, Bernardo Bottura, Luca Izquierdo Bermudez, Susana Löffler, Christian H Gomez, Jose V Lorenzo Savary, Frederic Probst, Matthias |
author_sort | Mangiarotti, Franco J |
collection | CERN |
description | A large number of training quenches at various currents, temperatures, and ramp rates, have been performed on six 11 T dipole model magnets. Quenches in the midplane of these magnets were of special interest, since the quench current in the last three models measured in 2016 was limited to between 84% and 92% of the magnets short sample limit. Measurements of quench propagation velocity, based on both voltage taps and quench antennas, yield a high propagation velocity of 50 to 80 m/s. Due to the high magnetic field gradient over the width of the midplane turn such a high propagation speed cannot be explained by propagation in longitudinal direction of the strand following the twist pitch. In these cases, current and heat sharing at the thin cable edge (where the field, stress, and cable compaction are high) are likely to provoke strand-to-strand quench propagation at higher velocities than along the strands. This investigation is focused on analyzing the quench propagation along the strands and strand-to-strand of various measured cases. |
id | oai-inspirehep.net-1669769 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2018 |
record_format | invenio |
spelling | oai-inspirehep.net-16697692019-09-30T06:29:59Zdoi:10.1109/TASC.2018.2818282http://cds.cern.ch/record/2674333engMangiarotti, Franco JWillering, Gerard PBajas, HuguesBajko, MartaBordini, BernardoBottura, LucaIzquierdo Bermudez, SusanaLöffler, Christian HGomez, Jose V LorenzoSavary, FredericProbst, MatthiasQuench propagation in Nb$_{3}$Sn cos-theta 11 T dipole model magnets in high stress areasAccelerators and Storage RingsA large number of training quenches at various currents, temperatures, and ramp rates, have been performed on six 11 T dipole model magnets. Quenches in the midplane of these magnets were of special interest, since the quench current in the last three models measured in 2016 was limited to between 84% and 92% of the magnets short sample limit. Measurements of quench propagation velocity, based on both voltage taps and quench antennas, yield a high propagation velocity of 50 to 80 m/s. Due to the high magnetic field gradient over the width of the midplane turn such a high propagation speed cannot be explained by propagation in longitudinal direction of the strand following the twist pitch. In these cases, current and heat sharing at the thin cable edge (where the field, stress, and cable compaction are high) are likely to provoke strand-to-strand quench propagation at higher velocities than along the strands. This investigation is focused on analyzing the quench propagation along the strands and strand-to-strand of various measured cases.oai:inspirehep.net:16697692018 |
spellingShingle | Accelerators and Storage Rings Mangiarotti, Franco J Willering, Gerard P Bajas, Hugues Bajko, Marta Bordini, Bernardo Bottura, Luca Izquierdo Bermudez, Susana Löffler, Christian H Gomez, Jose V Lorenzo Savary, Frederic Probst, Matthias Quench propagation in Nb$_{3}$Sn cos-theta 11 T dipole model magnets in high stress areas |
title | Quench propagation in Nb$_{3}$Sn cos-theta 11 T dipole model magnets in high stress areas |
title_full | Quench propagation in Nb$_{3}$Sn cos-theta 11 T dipole model magnets in high stress areas |
title_fullStr | Quench propagation in Nb$_{3}$Sn cos-theta 11 T dipole model magnets in high stress areas |
title_full_unstemmed | Quench propagation in Nb$_{3}$Sn cos-theta 11 T dipole model magnets in high stress areas |
title_short | Quench propagation in Nb$_{3}$Sn cos-theta 11 T dipole model magnets in high stress areas |
title_sort | quench propagation in nb$_{3}$sn cos-theta 11 t dipole model magnets in high stress areas |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.1109/TASC.2018.2818282 http://cds.cern.ch/record/2674333 |
work_keys_str_mv | AT mangiarottifrancoj quenchpropagationinnb3sncostheta11tdipolemodelmagnetsinhighstressareas AT willeringgerardp quenchpropagationinnb3sncostheta11tdipolemodelmagnetsinhighstressareas AT bajashugues quenchpropagationinnb3sncostheta11tdipolemodelmagnetsinhighstressareas AT bajkomarta quenchpropagationinnb3sncostheta11tdipolemodelmagnetsinhighstressareas AT bordinibernardo quenchpropagationinnb3sncostheta11tdipolemodelmagnetsinhighstressareas AT botturaluca quenchpropagationinnb3sncostheta11tdipolemodelmagnetsinhighstressareas AT izquierdobermudezsusana quenchpropagationinnb3sncostheta11tdipolemodelmagnetsinhighstressareas AT lofflerchristianh quenchpropagationinnb3sncostheta11tdipolemodelmagnetsinhighstressareas AT gomezjosevlorenzo quenchpropagationinnb3sncostheta11tdipolemodelmagnetsinhighstressareas AT savaryfrederic quenchpropagationinnb3sncostheta11tdipolemodelmagnetsinhighstressareas AT probstmatthias quenchpropagationinnb3sncostheta11tdipolemodelmagnetsinhighstressareas |