Quench detection for Mutiplerts: Introduction

Slides:



Advertisements
Similar presentations
The HiLumi LHC Design Study (a sub-system of HL-LHC) is co-funded by the European Commission within the Framework Programme 7 Capacities Specific Programme,
Advertisements

Neutron Irradiation Measurement for Superconducting Magnet Materials at Low Temperature Tatsushi NAKAMOTO KEK.
Cryogenic Experts Meeting (19 ~ ) Helium distribution system for Super-FRS dipoles and multiplets MT/FAIR – Cryogenics and Magnets Y. Xiang,
A payload to test in space Superconductive Magnetic Shielding technology R. Battiston Perugia University June 2010.
Superconducting Magnet R&D for COMET Makoto Yoshida (KEK) NuFact Aug, 2011.
This material is based upon work supported by the U.S. Department of Energy Office of Science under Cooperative Agreement DE-SC , the State of Michigan.
Superconducting Links for accelerator technology A.Ballarino CERN, TE-MSC-SCD Eucard’13, CERN With contributions from the SCD SL Team (B.Bordini, S.Giannelli),
REVIEW OF THE CRYOGENIC BY-PASS FOR THE LHC DS COLLIMATORS ELECTRICAL CIRCUIT MODIFICATION, INCLUDING OPERATIONAL CONSIDERATIONS PRESENTED BY A. SIEMKO.
DC-DC Buck Converter in Inner Detector Environment
Prospects of SC Quadrupole Production at IHEP-Protvino The 2nd Institutes Meeting on International Construction of the FAIR Accelerator Complex Protvino,
Solenoid-Based Focusing Lens for a Superconducting RF Proton Linac Presentation prepared for AEM 11/08/20101I. Terechkine.
Radiation damage effects on RRR WAMSDO 2013, 15./16.1., CERN René Flükiger CERN WAMSDO 2013, 15./ , CERN1.
HQ TEST CERN by Marta Bajko CERN TE-MSC TF For Hi Lumi and LARP the 16 th of November 2011 CERN.
Possible HTS wire implementation Amalia Ballarino Care HHH Working Meeting LHC beam-beam effects and beam-beam interaction CERN, 28 th August 2008.
Loss problems associated with the acceleration of radioactive beams and what we can do about it A.Jansson f fermilab Loss issues (and ideas for solutions)
IHEP participation in SIS300 production UNILAC SIS 18 SIS 100/300 HESR Super FRS NESR CR RESR Institute for High Energy Physics Protvino, Russia FAIR meeting.
September 19/20, 2007 SIS 100 Magnet cooling and cryogenic distribution.
Cryogenic Experts Meeting (19 ~ ) Cooling scheme discussion for 300 Tm High Energy Beam Transfer line (HEBT) with large inclination MT/FAIR –
The HiLumi LHC Design Study is included in the High Luminosity LHC project and is partly funded by the European Commission within the Framework Programme.
A. Verweij, TE-MPE. 3 Feb 2009, LHC Performance Workshop – Chamonix 2009 Arjan Verweij TE-MPE - joint stability - what was wrong with the ‘old’ bus-bar.
1 Second LHC Splice Review Copper Stabilizer Continuity Measurement possible QC tool for consolidated splices H. Thiesen 28 November 2011 K. Brodzinski,
Bock_DE_Session1_Block1_Question3 Barcelona May 2003 Nexans SuperConductors Dr. Joachim Bock Nexans SuperConductors D Huerth
Power Distribution Existing Systems Power in the trackers Power in the calorimeters Need for changes.
Big Magnet Design II: a) solenoid and cable concept b) short section test V.V. Kashikhin and A.V. Zlobin.
Review-LHC Interaction Regions - Upgrade Phase I Amalia Ballarino, 31 st July 2008 Cold Powering Options Conceptual Design Review of the LHC Interaction.
19./20. September 2007 Current leads for FAIR Cryogenic Expert Meeting 19./20. September 2007 Birgit Weckenmann.
SIS 300 Magnet Design Options. Cos n  magnets; cooling with supercritical Helium GSI 001 existing magnet built at BNG measured in our test facility 6.
AT-MEI-PE, RD, LIUWG 31-JUL R. Denz AT-MEI-PE LHC Luminosity Upgrade Protection of the Inner Triplet, D1, Correctors and Superconducting Links/Leads.
Arjan Verweij, AT-MAS, Workshop on test facilities and measurement equipment needed for the LHC exploitation, 12 April 2006 B163 - FRESCA.
Muon Cooling Channel Superconducting Magnet Systems Muon Collider Task Force Meeting on July 31, 2006 V.S. Kashikhin.
5 th Joint Hi-Lumi LHC-LARP Annual Meeting 2015 SC Link Protection A.Ballarino 28/10/2015.
Power Converters and DC cablesSlide 1/.. LHC - HC review Hugues THIESEN – AB/PO Thursday, 12 May 2005 Water cooled cables warm bus bars power converter.
Superconducting Technologies for the Next Generation of Accelerators CERN, Globe of Science and Innovation 4-5 December Superconducting Links for the Hi-Lumi.
The integration of 420 m detectors into the LHC
Mike Struik / LHC-CRI INSTRUMENTATION FEEDTHROUGH SYSTEM FOR LHC MACHINE ARC QUADRUPOLE MAGNETS. 123rd LHC Vacuum Design Meeting 19 April 1999.
TE-MPE participation on the GSI-CERN Collaboration for Testing Super-FRS's Superconducting Magnets (aka FAIR project) Daniel Calcoen Acknowledgements:
The HiLumi LHC Design Study (a sub-system of HL-LHC) is co-funded by the European Commission within the Framework Programme 7 Capacities Specific Programme,
Super Fragment Separator (Super-FRS) Machine and Magnets H. Leibrock, GSI Darmstadt Review on Cryogenics, February 27th, 2012, GSI Darmstadt.
TEST FACILITY STATUS FOR TESTING CERN Marta Bajko WP10. EUCARD 2 Task 4 - HTS Magnet Tests, June 2015.
The Super-FRS Multiplet, Magnetic and Cryogenic requirements
SIS 100 Vacuum chamber Recooler String system Components
Task 5: High-Tc superconducting link Summary of work-package
Existing Prototype Test Facility (PTF) and planned Series Test Facility Schroeder, Claus Cryo-Review Darmstadt
HL-LHC IT STRING and Series test of SC link
D1 and D2 powering and protection
Quench Simulation at GSI
Powering LHC magnets version 30/3/2007.
Testing of SC Magnets Status - November 2010
National Research Center” Kurchatov Institute”
The HL-LHC Circuits: Global View and Open Questions
HFM Test Station Main Cryostat
LHC Hardware Commissionning
INTER UNIVERSITY ACCELERATOR CENTER, INDIA
12 October 2009 RRB Plenary R.-D. Heuer
Long Shutdown for the LHC: Vacuum Beam Pipes
Powering the LHC Magnets
Update on circuit protection simulations of the HL-LHC Inner Triplet circuit Matthias Mentink, Circuit specifics + STEAM simulations: Samer Yammine, LEDET.
Circuits description and requirements - Closed Session-
Detailed global view on protection and detection of the circuits
EuCARD2 WP 10.2 HTS Conductor
3 issues identified in review
Collimator Control (SEUs & R2E Outlook)
Preliminary study of HTS option for CEPC detector magnet
The superconducting solenoids for the Super Charm-Tau Factory detector
Simulating Quench Signals in the LHC Superconducting Dipoles
Quench calculations of the CBM magnet
Analysis on Solenoidal High Temperature Superconducting Magnet using COMSOL MultiPhysics® Abhinav Kumar Department of Mechanical Engineering, Lovely Professional.
Power Leads for Test Stands
J. Fleiter, S. C. Hopkins, A. Ballarino
Assessment of stability of fully-excited Nb3Sn Rutherford cable with modified ICR at 4.2 K and 12 T using a superconducting transformer and solenoidal.
Presentation transcript:

Quench detection for Mutiplerts: Introduction - The Super-FRS and its magnets - 2 options for multiplet magnets: low current (I < 600 A), high current (I > 1000 A) - Options for powering the magnet: - local copper current leads (low and high current) - local HTS current leads (high current) - superconducting bypass line with copper current leads (high current) - superconducting bypass line with HTS current leads (high current) - Cost of quench detection for the different options - Basic characteristics of the superconducting bypass line - Radiation hardness of HTS current leads - Conclusions E. Floch. FAIR/MT. 22 Jan09

162 magnets distributed in 30 cryostats Super-FRS magnets dipole quadrupole (long) (short) octupole hexapole Steerers total 28 22 46 40 42 12 190 224 A 162 magnets distributed in 30 cryostats E. Floch. FAIR/MT. 22 Jan09

Local Copper current leads "Local current leads" means located inside one multiplet cryostat This option is : - that considered in the FBTR - valid for I < 300 A and could also be used for I up to 3 kA - the simplest, the most reliable and cheapest for quench detection E. Floch. FAIR/MT. 22 Jan09

Local HTS current leads Quench detection for one HTS lead is more complex and cost 826 € extra per lead (268 k€ extra for 162 magnets without voltage taps cabling) E. Floch. FAIR/MT. 22 Jan09

SC bypass line with Cu leads Only for high current option One extra bridge per magnet is needed to detect a quench in the superconducting bus bars ( 122 k€ extra for 162 magnets without voltage taps cabling) E. Floch. FAIR/MT. 22 Jan09

SC bypass line with HTS leads Only for high current option One extra bridge per magnet is needed to detect a quench in the superconducting bus bars ( 122 k€ extra for 162 magnets without voltage taps cabling) Quench detection for one HTS lead is more complex and cost 826 € extra per lead (268 k€ extra for 162 magnets without voltage taps cabling) E. Floch. FAIR/MT. 22 Jan09

Extra cost for quench detection Option (28 dipoles and 162 magnets in multiplets) bridges for magnets Bridges for bus bars CLQD1 (Cu leads) CLQD2 (HTS leads) quench control sys (k€) Voltage taps cabling (k€) Total Cost (k€) extra cost (k€) Cu local current leads 190 380 20 60 289 local HTS leads 56 324 108 604 316 Bypass line + Cu leads 162 194 545 256 Bypass line + HTS leads 350 968 679 E. Floch. FAIR/MT. 22 Jan09

SC bypass line Very probably: - the bypass line will be independent of the He supply line - 3 cooling schemes (magnets, bypass line, current lead boxes) are required - 4 extra feed through per magnet - 10 extra junctions (sc/sc or sc/Cu) per magnet E. Floch. FAIR/MT. 22 Jan09

SC bypass line: branches in sc joints - For a rigid SC bypass line that has 5 branches and feeds 30 cryostats, we can imagine to build it in 50 pieces - Each bypass line piece is different (length, n° of bus bars, and maybe diameter) - At the junction between 2 pieces, we will have to make on average 162 joints - We can estimate that the bypass line requires 9720 (162*50 +10*162) sc joints more than the option with local current leads (difficulty to locate a bad sc joint) - Such a Bypass line could cost several M€ E. Floch. FAIR/MT. 22 Jan09

Radiation harness of Bi223 LHC HTS current leads use Bi2223 tape with Ag matrix Irradiation of Bi2223 tape with Ag matrix Ref Protectile Energy (MeV) Fluence (projectile/cm2) Irradiation at Ic_irradiated / Ic_vergin 1 neutrons 17 (average) 1015 77 K 2*1015 300 K 1.02 2 protons 50 5*1017 0.3 Ref 1 : Ballarino, A. et al., “Effect of fast neutron irradiation on current transport properties of HTS materials”, http://at-mel-cf.web.cern.ch/at-mel-cf/resources/Irradiation_tests_Eucas.pdf. Ref 2 : A. F. Zeller, R. M. Ronningen, A. Godeke, L. H. Heilbronn, P. McMahan-Norris, and R. Gupta. "RADIATION DAMAGE TO BSCCO-2223 FROM 50 MEV PROTONS ", ICMC 2008 proceeding, p416-422. see http://proceedings.aip.org/proceedings/cpcr.jsp Before deciding to use HTS local current leads, one must be sure that the HTS tapes can withstand the expected radiation level in the Super-FRS E. Floch. FAIR/MT. 22 Jan09

Conclusions - For the high current option, we could think of a superconducting bypass line. - Such a SC bypass line has the following drawbacks: complex design (at least 50 individual pieces), 2 extra cooling schemes, 648 feed through, about 10 000 SC joints, quench detection cost would increase from 290 to 970 k€ - Because of all these disadvantages, the SC bypass line should be avoided - The simplest, most reliable and cheapest solution is to use local copper current leads - which is perfectly appropriate for I < 300 A - could be imagined even for higher current - In case HTS current leads are chosen (to lower cryogenic losses), one must be sure that the radiaton level in the Super-FRS is not dammaging the Bi2223 tape. E. Floch. FAIR/MT. 22 Jan09