Hovedsiden > Superconducting Magnet with the Minimum Steel Yoke for the Hadron Future Circular Collider Detector |
Article | |
Report number | arXiv:1605.08777 |
Title | Superconducting Magnet with the Minimum Steel Yoke for the Hadron Future Circular Collider Detector |
Author(s) | Klyukhin, V.I. (SINP, Moscow) ; Hervé, A. (U. Wisconsin, Madison (main)) ; Ball, A. (CERN) ; Curé, B. (CERN) ; Dudarev, A. (CERN) ; Gaddi, A. (CERN) ; Gerwig, H. (CERN) ; Mentink, M. (CERN) ; Da Silva, H. Pais (CERN) ; Rolando, G. (CERN) ; ten Kate, H. H. J. (CERN) ; Berriaud, C.P. (IRFU, Saclay) |
Publication | 2016 |
Imprint | 27 May 2016 |
Number of pages | 8 |
Note | 8 pages, 6 figures, presented at ICSM2016 - 5th International Conference on Superconductivity and Magnetism on April 26, 2016 at Fethiye, Turkey |
In: | J. Supercond. Novel Magn. 29 (2016) 3660 |
In: | 5th International Conference on Superconductivity and Magnetism, Fethiye, Turkey, 24 - 30 Apr 2016, pp.3660 |
DOI | 10.1007/s10948-016-3660-6 |
Subject category | Detectors and Experimental Techniques |
Abstract | 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. |
Copyright/License | arXiv nonexclusive-distrib. 1.0 publication: © 2016-2024 The Author(s) (License: CC-BY-4.0) |