Cargando…

Superconducting Magnet with the Minimum Steel Yoke for the Hadron Future Circular Collider Detector

The conceptual design study of a hadron Future Circular Collider (FCC-hh) with a center-of-mass energy of the order of 100 TeV in a new tunnel of 80-100 km circumference assumes the determination of the basic requirements for its detectors. A superconducting solenoid magnet of 12 m diameter inner bo...

Descripción completa

Detalles Bibliográficos
Autores principales: Klyukhin, V.I., Hervé, A., Ball, A., Curé, B., Dudarev, A., Gaddi, A., Gerwig, H., Mentink, M., Da Silva, H. Pais, Rolando, G., ten Kate, H. H. J., Berriaud, C.P.
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1007/s10948-016-3660-6
http://cds.cern.ch/record/2156862
_version_ 1780950696547319808
author Klyukhin, V.I.
Hervé, A.
Ball, A.
Curé, B.
Dudarev, A.
Gaddi, A.
Gerwig, H.
Mentink, M.
Da Silva, H. Pais
Rolando, G.
ten Kate, H. H. J.
Berriaud, C.P.
author_facet Klyukhin, V.I.
Hervé, A.
Ball, A.
Curé, B.
Dudarev, A.
Gaddi, A.
Gerwig, H.
Mentink, M.
Da Silva, H. Pais
Rolando, G.
ten Kate, H. H. J.
Berriaud, C.P.
author_sort Klyukhin, V.I.
collection CERN
description The conceptual design study of a hadron Future Circular Collider (FCC-hh) with a center-of-mass energy of the order of 100 TeV in a new tunnel of 80-100 km circumference assumes the determination of the basic requirements for its detectors. A superconducting solenoid magnet of 12 m diameter inner bore with the central magnetic flux density of 6 T in combination with two superconducting dipole and two conventional toroid magnets is proposed for a FCC-hh experimental setup. The coil of 23.468 m long has seven 3.35 m long modules included into one cryostat. The steel yoke with a mass of 22.6 kt consists of two barrel layers of 0.5 m radial thickness, and the 0.7 m thick nose disk and four 0.6 m thick end-cap disks each side. The maximum outer diameter of the yoke is 17.7 m; the length is 62.6 m. The air gaps between the end-cap disks provide the installation of the muon chambers up to the pseudorapidity about \pm 2.7. The superconducting dipole magnets allow measuring the charged particle momenta in the pseudorapidity region greater than \pm 3. The conventional forward muon spectrometers provide the muon identification in the pseudorapidity region from \pm 2.7 to \pm 5. The magnet modeled with Cobham's program TOSCA. The total current in the superconducting solenoid coil is 123 MA-turns; the stored energy is 41.8 GJ. The axial force onto each end-cap is 450 MN. The stray field at the radius of 50 m off the coil axis is 13.7 mT and 5.2 mT at the radius of 100 m. All other parameters presented and discussed.
id cern-2156862
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2016
record_format invenio
spelling cern-21568622023-05-05T02:07:15Zdoi:10.1007/s10948-016-3660-6http://cds.cern.ch/record/2156862engKlyukhin, V.I.Hervé, A.Ball, A.Curé, B.Dudarev, A.Gaddi, A.Gerwig, H.Mentink, M.Da Silva, H. PaisRolando, G.ten Kate, H. H. J.Berriaud, C.P.Superconducting Magnet with the Minimum Steel Yoke for the Hadron Future Circular Collider DetectorDetectors and Experimental TechniquesThe conceptual design study of a hadron Future Circular Collider (FCC-hh) with a center-of-mass energy of the order of 100 TeV in a new tunnel of 80-100 km circumference assumes the determination of the basic requirements for its detectors. A superconducting solenoid magnet of 12 m diameter inner bore with the central magnetic flux density of 6 T in combination with two superconducting dipole and two conventional toroid magnets is proposed for a FCC-hh experimental setup. The coil of 23.468 m long has seven 3.35 m long modules included into one cryostat. The steel yoke with a mass of 22.6 kt consists of two barrel layers of 0.5 m radial thickness, and the 0.7 m thick nose disk and four 0.6 m thick end-cap disks each side. The maximum outer diameter of the yoke is 17.7 m; the length is 62.6 m. The air gaps between the end-cap disks provide the installation of the muon chambers up to the pseudorapidity about \pm 2.7. The superconducting dipole magnets allow measuring the charged particle momenta in the pseudorapidity region greater than \pm 3. The conventional forward muon spectrometers provide the muon identification in the pseudorapidity region from \pm 2.7 to \pm 5. The magnet modeled with Cobham's program TOSCA. The total current in the superconducting solenoid coil is 123 MA-turns; the stored energy is 41.8 GJ. The axial force onto each end-cap is 450 MN. The stray field at the radius of 50 m off the coil axis is 13.7 mT and 5.2 mT at the radius of 100 m. All other parameters presented and discussed.The conceptual design study of a Future Circular hadron-hadron Collider (FCC-hh) with a center-of-mass energy of the order of 100 TeV, assumed to be constructed in a new tunnel of 80-100 km circumference, includes the determination of the basic requirements for its detectors. A superconducting solenoid magnet of 12-m-diameter inner bore with the central magnetic flux density of 6 T, in combination with two superconducting dipole magnets and two conventional toroid magnets is proposed for an FCC-hh experimental setup. The coil of 23.468 m length has seven 3.35-m-long modules included into one cryostat. The steel yoke with a mass of 22.6 kt consists of two barrel layers of 0.5 m radial thickness and a 0.7-m-thick nose disk and four 0.6-m-thick end-cap disks each side. The outer diameter of the yoke is 17.7 m. The full length of the magnetic system is 62.6 m. The air gaps between the end-cap disks provide for the installation of the muon chambers up to an absolute pseudorapidity about 2.7. The superconducting dipole magnets provide measurement of charged particle momenta in the absolute pseudorapidity region greater than 3. The conventional forward muon spectrometer allows muon identification in the absolute pseudorapidity region from 2.7 to 5. The magnet is modeled with the program TOSCA from Cobham CTS Limited. The total current in the superconducting solenoid coil is 123 MA-turns; the stored energy is 41.8 GJ. The axial force acting on each end-cap is 450 MN. The stray field is 13.7 mT at a radius of 50 m from the coil axis, and 5.2 mT at a radius of 100 m. Many other parameters are presented and discussed.arXiv:1605.08777oai:cds.cern.ch:21568622016-05-27
spellingShingle Detectors and Experimental Techniques
Klyukhin, V.I.
Hervé, A.
Ball, A.
Curé, B.
Dudarev, A.
Gaddi, A.
Gerwig, H.
Mentink, M.
Da Silva, H. Pais
Rolando, G.
ten Kate, H. H. J.
Berriaud, C.P.
Superconducting Magnet with the Minimum Steel Yoke for the Hadron Future Circular Collider Detector
title Superconducting Magnet with the Minimum Steel Yoke for the Hadron Future Circular Collider Detector
title_full Superconducting Magnet with the Minimum Steel Yoke for the Hadron Future Circular Collider Detector
title_fullStr Superconducting Magnet with the Minimum Steel Yoke for the Hadron Future Circular Collider Detector
title_full_unstemmed Superconducting Magnet with the Minimum Steel Yoke for the Hadron Future Circular Collider Detector
title_short Superconducting Magnet with the Minimum Steel Yoke for the Hadron Future Circular Collider Detector
title_sort superconducting magnet with the minimum steel yoke for the hadron future circular collider detector
topic Detectors and Experimental Techniques
url https://dx.doi.org/10.1007/s10948-016-3660-6
http://cds.cern.ch/record/2156862
work_keys_str_mv AT klyukhinvi superconductingmagnetwiththeminimumsteelyokeforthehadronfuturecircularcolliderdetector
AT hervea superconductingmagnetwiththeminimumsteelyokeforthehadronfuturecircularcolliderdetector
AT balla superconductingmagnetwiththeminimumsteelyokeforthehadronfuturecircularcolliderdetector
AT cureb superconductingmagnetwiththeminimumsteelyokeforthehadronfuturecircularcolliderdetector
AT dudareva superconductingmagnetwiththeminimumsteelyokeforthehadronfuturecircularcolliderdetector
AT gaddia superconductingmagnetwiththeminimumsteelyokeforthehadronfuturecircularcolliderdetector
AT gerwigh superconductingmagnetwiththeminimumsteelyokeforthehadronfuturecircularcolliderdetector
AT mentinkm superconductingmagnetwiththeminimumsteelyokeforthehadronfuturecircularcolliderdetector
AT dasilvahpais superconductingmagnetwiththeminimumsteelyokeforthehadronfuturecircularcolliderdetector
AT rolandog superconductingmagnetwiththeminimumsteelyokeforthehadronfuturecircularcolliderdetector
AT tenkatehhj superconductingmagnetwiththeminimumsteelyokeforthehadronfuturecircularcolliderdetector
AT berriaudcp superconductingmagnetwiththeminimumsteelyokeforthehadronfuturecircularcolliderdetector