BNL High Field and HTS Magnet Program Ramesh Gupta BNL, NY USA H T.

Slides:



Advertisements
Similar presentations
Superconducting Magnet Program S. Gourlay CERN March 11-12, Lawrence Berkeley National Laboratory IR Quad R&D Program LHC IR Upgrade Stephen A.
Advertisements

Ramesh Gupta, BNL D1 Dipole Design / IR Magnet Study LARP Collaboration Meeting, Oct 5-6, D1 Dipole Design Task (terminated in 2005) IR Magnet Study.
D2 conceptual design and field quality optimization Ramesh Gupta, BNL Slide No. 1 Nov. 13, 2013 D2 Conceptual Design and Field Quality.
September 2007 FP7-IA HFM JRA proposal G. de Rijk (CERN)1 FP7-IA HFM JRA proposal   The proposal is under discussion: we welcome input from potential.
Undulator R & D Jim Clarke STFC Daresbury Laboratory, UK BAW-2 SLAC Jan 2011.
11 September 2007 FP7-IA HFM JRA proposal G. de Rijk (CERN)1 FP7-IA HFM JRA proposal   Outline Motivation General description Proposed Work Packages.
Optimisation of Roebel cable for HTS accelerator magnets
HTS Coils for High Field Hybrid FCC Dipoles Ramesh Gupta March 23-27, Superconducting Magnet Division HTS Coils for High Field Hybrid FCC Dipoles.
Report from WAMHTS-2 and opportunities for HTS Naoyuki Amemiya Kyoto University 1.
Aug 29, 2006S. Kahn T HTS Solenoid1 A Proposal for a 50 T HTS Solenoid Steve Kahn Muons Inc. August 29, 2006.
Development of Superconducting Magnets for Particle Accelerators and Detectors in High Energy Physics Takakazu Shintomi and Akira Yamamoto On behalf of.
Superconducting Large Bore Sextupole for ILC
Progress Towards A High-field HTS Solenoid
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.
MCTF Alexander Zlobin MUTAC Meeting 8-10 April MCTF Magnet and HTS Conductor R&D.
Superconducting Magnet Division Ramesh Gupta High Field Magnet R&D with YBCO July 26, 2011Slide No. 1 EUCARD2 VIDEO CONFERENCE.
MCTF Michael Lamm MUTAC 5-Year Plan Review 22 August Magnet R&D for Muon Accelerator R&D Program Goals Proposed Studies Preliminary Effort and Cost.
EuCARD2 Magnet Status and action plan
FCC Week 2015Design Options for 16 T LTS Dipoles – G. Sabbi 1 Overview of Magnet Design Options for LTS Dipoles in the 16 T Range GianLuca Sabbi, LBNL.
Magnets for muon collider ring and interaction regions V.V. Kashikhin, FNAL December 03, 2009.
Qingjin XU Institute of High Energy Physics (IHEP)
Superconducting R&D – Now Strand and Cable R&D FERMILAB Magnet Systems Department – Now SC Materials Department (TD) HTS Insert Coil Test in External Solenoid.
Towards Nb 3 Sn accelerator magnets, challenges & solutions, history & forecast Shlomo Caspi Superconducting Magnet Group Lawrence Berkeley National Laboratory.
Development of the EuCARD Nb 3 Sn Dipole Magnet FRESCA2 P. Ferracin, M. Devaux, M. Durante, P. Fazilleau, P. Fessia, P. Manil, A. Milanese, J. E. Munoz.
EuCARD-2 is co-funded by the partners and the European Commission under Capacities 7th Framework Programme, Grant Agreement EuCARD-2 WP-10 Status.
11 T Nb3Sn Demonstrator Dipole R&D Strategy and Status
Bnl - fnal- lbnl - slac US LHC Accelerator Research Program A Quadrupole Design for Crab Cavity Optics Ramesh Gupta Brookhaven National Laboratory Upton,
ASC 2014Nb 3 Sn Block Coil Dipoles for a 100 TeV Hadron Collider – G. Sabbi 1 Performance characteristics of Nb 3 Sn block-coil dipoles for a 100 TeV hadron.
S. Caspi, LBNL HQ Progress and Schedule Shlomo Caspi LBNL LARP Collaboration Meeting – CM13 Port Jefferson November 4-6, 2009.
Superferric CEA. CEA is involved in the FAIR/GSI project: Responsible for the conceptual design preparation and technical follow-up of 24 superferric.
Superconducting Corrector Magnet Progress Report P. Wanderer Superconducting Magnet Div; Dec. 15, 2007 T2K US B280 collaboration meeting.
G.A.Kirby 4th Nov.08 High Field Magnet Fresca 2 Introduction Existing strand designs, PIT and OST’s RRP are being used in the conceptual designs for two.
S. Gourlay 7/19/01 T2 Working Group Summary T2 Working Group Summary Magnet Technology: Permanent Magnets, Superconducting Magnets, Power Supplies Conveners:
Open Midplane Dipole (OMD) Design for Dipole First Layout R. Gupta (BNL), N. Mokhov (FANL) bnl - fnal- lbnl - slac US LHC Accelerator Research Program.
Harold G. Kirk Brookhaven National Laboratory High-Field Solenoids for a MC Final Cooling System AAC 2012 Austin, Texas June 11-15, 2012.
Dipole design at the 16 T frontier - Magnet R&D for a Future Circular Collider (FCC) at Fermilab Alexander Zlobin Fermilab.
HTS High-Field Solenoid Development March xx, 2013 Presenter’s Name | DOE Mini-Review of MAP (FNAL, March 4-6, 2013)1 Advanced Quench Protection System.
Magnet R&D for Muon Beam Cooling at FNAL Alexander Zlobin Fermilab Muon Collider Design Workshop, BNL December 1-3, 2009.
JRA on Development of High Temperature SC Link Motivation Work Packages Partners & resources Amalia Ballarino Esgard open meeting CERN,
Helical Solenoid Development
Prospects for the use of HTS in high field magnets for future accelerator facilities A. Ballarino CERN, Geneva, Switzerland.
Next Steps in Magnet R&D Steve Gourlay LBNL EuCARD Workshop on a High Energy LHC Malta October 14, 2010.
FCC EuroCirCol kick-off,CERN, 3 rd June 2015.
1 BNL -FNAL - LBNL - SLAC P. Wanderer IR’07 - Frascati 7 November 2007 U.S. LARP Magnet Programme.
Report from Session 2 Main Dipoles. P. McIntyre 2005 – 24T ss Tripler, a lot of Bi-2212, Je = 800 A/mm2 E. Todesco T, 80% ss 30% NbTi 55 %NbSn.
1 1 Office of Science Steve Gourlay August 13, 2014 LBNL Superconducting Magnet Program High Energy Physics.
Program overview: motivation, target parameters, timeline A.V. Zlobin 15 T dipole design review 28 April 2016.
Superconducting Magnet Division Status of High Field Solenoid Development - Ramesh Gupta Slide No. 1 MAP13 June 19, 2013.
Study of the HTS Insert Quench Protection M. Sorbi and A. Stenvall 1 HFM-EuCARD, ESAC meeting, WP 7.4.1CEA Saclay 28 feb. 2013,
Magnet Strategy Michael Lamm Technical Division/Magnet Systems Department Fermilab Muon Accelerator Program Review Fermilab, August 25, 2010.
HTS and LTS Magnet Design and Prototyping for RAON
Hadron Collider Breakout Session Summary
Massimo Sorbi on behalf of INFN team:
CORC®: Results and Perspectives Danko van der Laan and Jeremy Weiss
At ICFA Mini-Workshop on High Field Magnets for pp Colliders,
High Field Hybrid Design
Q0 magnet, cooling, support ideas
Bore quench field vs. critical current density
Naoyuki Amemiya Kyoto University
HTS Magnet R&D at BNL Ramesh Gupta November 17, 2017.
HTS/LTS Hybrid Test Results and Common Coil Design Update
DESIGN OPTIONS IN THE T RANGE
High-field magnets wound from CORC® cables and wires
EuCARD2 WP 10.2 HTS Conductor
Ramesh Gupta Brookhaven National Laboratory
PROGRESS TOWARDS AN OPEN MIDPLANE SEPARATION DIPOLE
Muon Collider Magnet Technologies/Challenges
Muon Collider SR and IR Magnets
Qingjin XU Institute of High Energy Physics (IHEP),
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:

BNL High Field and HTS Magnet Program Ramesh Gupta BNL, NY USA H T

HTS Magnet Program at BNL HTS magnet R&D over a wide range: High field, Medium field and low field (high temperature) Many geometries – racetrack, cosine theta, solenoid Number of HTS coils/magnets designed built & tested: Well over 100 HTS coils and well over 10 HTS magnets Type of HTS used: Bi2223, Bi2212, ReBCO, MgB2 – wire, cable, tape Amount of HTS acquired: ~50 km (4 mm tape equivalent) Or recent activities have been largely on magnets with ReBCO (yet one Bi2223 and one MgB2 magnet is ready for testing)

Superconducting Magnetic Energy Storage (SMES) Key Target Parameters: 25T, 100mm, 1.7MJ, 12mm ReBCO High field large aperture HTS solenoid with huge stresses Ramesh Gupta, BNL, Aug 2014 Funded by arpa-e as a “high risk, high reward” project 3

HTS Magnet Test Results (BNL/ABB/SuperPower/Houston) 100 mm bore ReBCO ARPA- E SMES Coil 2 pancakes 1140 A, 4K 46 pancakes 350 A, 27K, 12.5 T 12 pancakes 760 A, 4K, 11.4 T Peak fields higher R. Gupta, BNL, Aug 2014

High Field HTS Magnet- PBL/BNL SBIR Field on axis: 15.7 T Field on coil : 16.2 T (original target: 10-12T) Highest field all HTS solenoid Overall Jo in coil: >500 A/mm2 @16 T Aperture = 25 mm *Credit to SBIR/STTR office for this and SMES work which was the result of this

2G HTS Quad for FRIB Fragment Separator Region Important: Magnet for a real machine- baseline design of FRIB

Large Temperature Margins (only possible with HTS) Provides robust operation against local and global heat loads

Advanced Quench Protection Electronics Detects onset of pre-quench voltage at < 1mV and with isolation voltage > 1kV allows fast energy extraction

Protection of HTS Magnet During an Operational Accident Near Design Current Design: 210 A in SP Coils 185A 175A Ringing in power supply made situation worse 90mV

Magnet Designs for FCC

Cos (q) Coil - PBL/BNL STTR#1 (12 mm, one block, 77 K) BENEFITS of Kapton-CI: No epoxy/adhesive to HTS tape (prone to degradation by epoxy) Standard insulation in magnets Cured coil can be handled easily Makes good coil (including ends) No measurable degradation@77 K

Cos (q) Coil - PBL/BNL STTR#2 (4 mm, goal: full coil, 4 K test) Future Plan (Phase I & Phase II) Construction and 4 K test of full cos (θ) coil in next few months R&D to develop base technology for accelerator magnets in next few years (includes measuring and finding ways to deal with magnetization) Use these magnets in an accelerator in next few decades No measurable degradation@77 K

High Field 2-in-1 Common Coil Dipole Design for Colliders Beam #1 Coil #1 Coil #2 Beam #2 Highest field R&W Nb3Sn dipole HTS tape common coil dipole A conductor friendly design Suitable for HTS coils – Roebel cable? Unfavorable orientation wrt field However, think long term. Will Ic remain so anisotropic forever?

A Coil Design with Overpass/Underpass Ends Optimized for ReBCO Tape R. Gupta, et al., “Next Generation IR Magnets for Hadron Colliders,” ASC2002 No need for lifting the ends and no reverse curvature Less strain on the conductor but winding more complicated Align ReBCO tape parallel to the field for Higher Jc Lower magnetization (will depend on the thickness and not on the width) Solenoid Type Ends

Magnet R&D for FCC

HTS coil become a part of the hybrid magnet test (~15 T) Common Coil Dipole at BNL for Testing HTS Insert Coils as in a Hybrid Magnet BNL has a unique 10+ T Nb3Sn common coil dipole with large open space to test HTS coils in background field. Provides fast turn around and economic R&D as no disassembly/assembly of the magnet is required HTS coil become a part of the hybrid magnet test (~15 T) High current 2212 coil

A Warm bore Cryo-cooled Magnet with 6 HTS coils Suitable for various studies Quench studies Measure magnetization induced harmonics as a function of time as a function of temperature as a function of field Evening: Switch ON; Morning: COLD BNL has about 50 HTS coils available for various studies; about 30 with ~100 meters of HTS Consider utilizing this asset

Summary Yet a long way to go before HTS magnets can be used in HEP accelerators, HTS magnet technology has made a major progress over last decade. (I’m personally optimistic). BNL has been active on developing HTS magnet technology and has made many significant demonstrations. BNL is looking forward to offer its unique and substantial experience to future HTS magnet R&D for FCC. However, we are more than HTS‘R’US (of which I’m proud of). We also have active programs on LTS magnets (our bread-and-better), and are the one US facility with working superconducting accelerator magnets.