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The bending magnets for the LHC injection transfer lines
Two injection transfer lines, each about 2.8 km long, with 51 and 107 degree horizontal deflection, are being built to transfer protons at 450 GeV from the Super Proton Synchrotron (SPS) to the Large Hadron Collider (LHC). A total of 360 dipole magnets are required; they have been produced in the fr...
Autores principales: | , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2002
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1109/TASC.2002.1018365 http://cds.cern.ch/record/590810 |
_version_ | 1780899653730959360 |
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author | Anashin, V Bulygin, A Labutsky, S A Mejidzade, V Mikhailov, S Pupkov, Yu A Rouvinsky, E Sukhina, B Kalbreier, Willi Kouba, G Schirm, K M Weisse, E Konstantinov, Yu S Kosjakin, M Peregud, V |
author_facet | Anashin, V Bulygin, A Labutsky, S A Mejidzade, V Mikhailov, S Pupkov, Yu A Rouvinsky, E Sukhina, B Kalbreier, Willi Kouba, G Schirm, K M Weisse, E Konstantinov, Yu S Kosjakin, M Peregud, V |
author_sort | Anashin, V |
collection | CERN |
description | Two injection transfer lines, each about 2.8 km long, with 51 and 107 degree horizontal deflection, are being built to transfer protons at 450 GeV from the Super Proton Synchrotron (SPS) to the Large Hadron Collider (LHC). A total of 360 dipole magnets are required; they have been produced in the framework of the contribution of the Russian Federation to the construction of the LHC. The classical dipoles, built from laminated steel cores and copper coils, have a core length of 6.3 m, 25 mm gap height and a nominal field of 1.81 T at a current of 5270 A. The magnet design was made in collaboration between CERN and BINP. An unusual design has been chosen for the coils to cope with the limited voltage from the available power supplies. All magnets in each of the two lines will be powered in series. The coil is composed of overlapping, but electrically insulated, half coils of 3 1/2 turns each. Thus, the power connections for IN and OUT are placed on opposite magnet ends. Short copper braids are used to connect all upper or lower half coils in series and the whole string can be powered without power consuming cable links running alongside the magnets. Precautions are taken to avoid transmission line effects and hazards from differences in voltage between upper and lower half coil. Advantages and drawbacks of this concept are discussed as well as results of the acceptance test including mechanical, electrical and magnetic field measurements. Fabrication and measurement of the magnets at BINP, with the half core production subcontracted to EFREMOV, have been finished in June 2001. (9 refs). |
id | cern-590810 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2002 |
record_format | invenio |
spelling | cern-5908102019-09-30T06:29:59Zdoi:10.1109/TASC.2002.1018365http://cds.cern.ch/record/590810engAnashin, VBulygin, ALabutsky, S AMejidzade, VMikhailov, SPupkov, Yu ARouvinsky, ESukhina, BKalbreier, WilliKouba, GSchirm, K MWeisse, EKonstantinov, Yu SKosjakin, MPeregud, VThe bending magnets for the LHC injection transfer linesAccelerators and Storage RingsTwo injection transfer lines, each about 2.8 km long, with 51 and 107 degree horizontal deflection, are being built to transfer protons at 450 GeV from the Super Proton Synchrotron (SPS) to the Large Hadron Collider (LHC). A total of 360 dipole magnets are required; they have been produced in the framework of the contribution of the Russian Federation to the construction of the LHC. The classical dipoles, built from laminated steel cores and copper coils, have a core length of 6.3 m, 25 mm gap height and a nominal field of 1.81 T at a current of 5270 A. The magnet design was made in collaboration between CERN and BINP. An unusual design has been chosen for the coils to cope with the limited voltage from the available power supplies. All magnets in each of the two lines will be powered in series. The coil is composed of overlapping, but electrically insulated, half coils of 3 1/2 turns each. Thus, the power connections for IN and OUT are placed on opposite magnet ends. Short copper braids are used to connect all upper or lower half coils in series and the whole string can be powered without power consuming cable links running alongside the magnets. Precautions are taken to avoid transmission line effects and hazards from differences in voltage between upper and lower half coil. Advantages and drawbacks of this concept are discussed as well as results of the acceptance test including mechanical, electrical and magnetic field measurements. Fabrication and measurement of the magnets at BINP, with the half core production subcontracted to EFREMOV, have been finished in June 2001. (9 refs).oai:cds.cern.ch:5908102002 |
spellingShingle | Accelerators and Storage Rings Anashin, V Bulygin, A Labutsky, S A Mejidzade, V Mikhailov, S Pupkov, Yu A Rouvinsky, E Sukhina, B Kalbreier, Willi Kouba, G Schirm, K M Weisse, E Konstantinov, Yu S Kosjakin, M Peregud, V The bending magnets for the LHC injection transfer lines |
title | The bending magnets for the LHC injection transfer lines |
title_full | The bending magnets for the LHC injection transfer lines |
title_fullStr | The bending magnets for the LHC injection transfer lines |
title_full_unstemmed | The bending magnets for the LHC injection transfer lines |
title_short | The bending magnets for the LHC injection transfer lines |
title_sort | bending magnets for the lhc injection transfer lines |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.1109/TASC.2002.1018365 http://cds.cern.ch/record/590810 |
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