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Design of a Canted-cosine-theta orbit corrector for the High Luminosity LHC

The High Luminosity LHC requires dipole orbit correctors grouped in double aperture magnet assemblies. They provide a field of 3.1 T at 100 A in an aperture of 70 mm. The current standard design is a classical cosine-theta layout made with ribbon cable. However, the electric insulation of this cable...

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Autores principales: Pepitone, K., Kirby, G., Ruber, R., Ahl, A., Canale, M., Dugic, I., Gentini, L., Johansson, M., Karlsson, G., Kovacikova, J., Lindström, J., Olsson, A., Olvegård, M.
Lenguaje:eng
Publicado: 2022
Materias:
Acceso en línea:https://dx.doi.org/10.1109/TASC.2022.3154334
http://cds.cern.ch/record/2803347
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author Pepitone, K.
Kirby, G.
Ruber, R.
Ahl, A.
Canale, M.
Dugic, I.
Gentini, L.
Johansson, M.
Karlsson, G.
Kovacikova, J.
Lindström, J.
Olsson, A.
Olvegård, M.
author_facet Pepitone, K.
Kirby, G.
Ruber, R.
Ahl, A.
Canale, M.
Dugic, I.
Gentini, L.
Johansson, M.
Karlsson, G.
Kovacikova, J.
Lindström, J.
Olsson, A.
Olvegård, M.
author_sort Pepitone, K.
collection CERN
description The High Luminosity LHC requires dipole orbit correctors grouped in double aperture magnet assemblies. They provide a field of 3.1 T at 100 A in an aperture of 70 mm. The current standard design is a classical cosine-theta layout made with ribbon cable. However, the electric insulation of this cable is not radiation-resistant enough to withstand the radiation load expected in the coming years of LHC operation. A new design, based on a cable with polyimide insulator, that can replace the existing orbit correctors, is needed. The challenge is to design a magnet that fits directly into the existing positions and that can operate with the same busbars, passive quench protection, and power supplies. The new orbit corrector design meets high requirements on the field quality while keeping within the same mechanical volume and maximum excitation current. A collaboration of Swedish universities and Swedish industry has been formed for the development and production of a prototype magnet following a concurrent engineering methodology to reduce the time needed to produce a CCT magnet. The magnet has a 1 m long CCT dipole layout consisting of two coils. The superconductor is a commercially available 0.33 mm wire with polyimide insulation in a 6-around-1 cable. The channels in the coil formers, that determine the CCT layout, allow for <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$2\times 5$</tex-math></inline-formula> cable layers. A total of 70 windings makes that the coil current can be kept below 100 A. We will present the detailed design and preliminary quench simulations.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2022
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spelling cern-28033472023-03-14T07:58:29Zdoi:10.1109/TASC.2022.3154334http://cds.cern.ch/record/2803347engPepitone, K.Kirby, G.Ruber, R.Ahl, A.Canale, M.Dugic, I.Gentini, L.Johansson, M.Karlsson, G.Kovacikova, J.Lindström, J.Olsson, A.Olvegård, M.Design of a Canted-cosine-theta orbit corrector for the High Luminosity LHCAccelerators and Storage RingsThe High Luminosity LHC requires dipole orbit correctors grouped in double aperture magnet assemblies. They provide a field of 3.1 T at 100 A in an aperture of 70 mm. The current standard design is a classical cosine-theta layout made with ribbon cable. However, the electric insulation of this cable is not radiation-resistant enough to withstand the radiation load expected in the coming years of LHC operation. A new design, based on a cable with polyimide insulator, that can replace the existing orbit correctors, is needed. The challenge is to design a magnet that fits directly into the existing positions and that can operate with the same busbars, passive quench protection, and power supplies. The new orbit corrector design meets high requirements on the field quality while keeping within the same mechanical volume and maximum excitation current. A collaboration of Swedish universities and Swedish industry has been formed for the development and production of a prototype magnet following a concurrent engineering methodology to reduce the time needed to produce a CCT magnet. The magnet has a 1 m long CCT dipole layout consisting of two coils. The superconductor is a commercially available 0.33 mm wire with polyimide insulation in a 6-around-1 cable. The channels in the coil formers, that determine the CCT layout, allow for <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$2\times 5$</tex-math></inline-formula> cable layers. A total of 70 windings makes that the coil current can be kept below 100 A. We will present the detailed design and preliminary quench simulations.The High Luminosity LHC requires dipole orbit correctors grouped in double aperture magnet assemblies. They provide a field of 3.1 T at 100 A in an aperture of 70 mm. The current standard design is a classical cosine-theta layout made with ribbon cable. However, the electric insulation of the ribbon cable is not radiation-resistant enough to withstand the radiation load expected in the coming years of LHC operation. A new design, based on a radiation-resistant cable with polyimide insulator, that can replace the existing orbit correctors at their end-of-life, is needed. The challenge is to design a magnet that fits directly into the existing positions and that can operate with the same busbars, passive quench protection, and power supplies as existing magnets. We propose a self-protected canted-cosine-theta (CCT) design. We take the opportunity to explore new concepts for the CCT design to produce a cost-effective and high-quality design with a more sustainable use of resources. The new orbit corrector design meets high requirements on the field quality while keeping within the same mechanical volume and maximum excitation current. A collaboration of Swedish universities and Swedish industry has been formed for the development and production of a prototype magnet following a concurrent engineering (CE) methodology to reduce the time needed to produce a functional CCT magnet. The magnet has a 1 m long CCT dipole layout consisting of two coils. The superconductor is a commercially available 0.33 mm wire with polyimide insulation in a 6-around-1 cable. The channels in the coil formers, that determine the CCT layout, allow for 2 x 5 cable layers. A total of 70 windings makes that the coil current can be kept below 100 A. We will present the detailed design and preliminary quench simulations.arXiv:2202.10305oai:cds.cern.ch:28033472022-02-21
spellingShingle Accelerators and Storage Rings
Pepitone, K.
Kirby, G.
Ruber, R.
Ahl, A.
Canale, M.
Dugic, I.
Gentini, L.
Johansson, M.
Karlsson, G.
Kovacikova, J.
Lindström, J.
Olsson, A.
Olvegård, M.
Design of a Canted-cosine-theta orbit corrector for the High Luminosity LHC
title Design of a Canted-cosine-theta orbit corrector for the High Luminosity LHC
title_full Design of a Canted-cosine-theta orbit corrector for the High Luminosity LHC
title_fullStr Design of a Canted-cosine-theta orbit corrector for the High Luminosity LHC
title_full_unstemmed Design of a Canted-cosine-theta orbit corrector for the High Luminosity LHC
title_short Design of a Canted-cosine-theta orbit corrector for the High Luminosity LHC
title_sort design of a canted-cosine-theta orbit corrector for the high luminosity lhc
topic Accelerators and Storage Rings
url https://dx.doi.org/10.1109/TASC.2022.3154334
http://cds.cern.ch/record/2803347
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