Report from WAMHTS-1 in EuCARD2 CM

Slides:



Advertisements
Similar presentations
Superconductivity UK Dr. Philip Sargent, Diboride Conductors Ltd. Commercial superconductors, Cryogenics and Transformers.
Advertisements

Superconducting Magnet Program S. Gourlay CERN March 11-12, Lawrence Berkeley National Laboratory IR Quad R&D Program LHC IR Upgrade Stephen A.
E. Todesco DIPOLES FOR HIGH ENERGY LHC E. Todesco CERN, Geneva Switzerland Acknowledgements: B. Bordini, L. Bottura, G. De Rijk, L. Evans, P. Fessia, J.
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.
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
Preliminary Design of Nb 3 Sn Quadrupoles for FCC-hh M. Karppinen CERN TE-MSC.
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.
ARIES CS Magnet definition L. Bromberg MIT Plasma Science and Fusion Center USCD November 18, 2005.
Stellarator magnet conductors L. Bromberg J. Schultz MIT Plasma Science and Fusion Center Cambridge MA Aries Meeting, Georgia Tech September 3, 2003.
Applied superconductivity group L. García-Tabarés, F. Toral, I. RodriguezCIEMAT, I/2008.
Magnet costs L. Bromberg J.H. Schultz ARIES Meeting & Review PPPL, October
Superconducting Large Bore Sextupole for ILC
Roebel cable industrial optimization - General Cable Superconductors Dr Nick Long, Robinson Research Institute, Victoria University of Wellington, New.
Nb3Sn Cable and Insulation for LARP High-Gradient Quadrupole Magnets
Randy Tremper and Dean Peterson Los Alamos National Laboratory Los Alamos, New Mexico Superconductivity Technology Center Overview Develop Energy Efficient.
Innovation with Integrity Klaus Schlenga Washington, March 25, 2015 Bruker response to the FCC specifications.
Superconducting Magnet Division Ramesh Gupta High Field Magnet R&D with YBCO July 26, 2011Slide No. 1 EUCARD2 VIDEO CONFERENCE.
TFA-MOD derived YBa 2 Cu 3 O 7-x thick films assisted by a high magnetic field Wang H, Wang Q L, Huang H Li B L, Ma Y W, Yan L G Applied Superconductivity.
Possible HTS wire implementation Amalia Ballarino Care HHH Working Meeting LHC beam-beam effects and beam-beam interaction CERN, 28 th August 2008.
EuCARD2 Magnet Status and action plan
Magnets for muon collider ring and interaction regions V.V. Kashikhin, FNAL December 03, 2009.
The FCC Magnet Program: Challenges and Opportunities for HTS
EuCARD-2 is co-funded by the partners and the European Commission under Capacities 7th Framework Programme, Grant Agreement EuCARD-2 WP-10 Status.
Proposals of high efficiency accelerator components from AAA Green-ILC WG H. Hayano, KEK
11 T Nb3Sn Demonstrator Dipole R&D Strategy and Status
Current Activity And Future Effort.  High Tc Superconductor (HTS) magnet R&D  important for future high energy and/or high intensity accelerator applications.
FCC kick-off meeting a summary for magnets L. Bottura
FCC-related R&D in KEK and Japan
CERN Accelerator School Superconductivity for Accelerators Case study introduction Paolo Ferracin CERN, Geneva Claire Antoine
GROUP C – Case study no.4 Dr. Nadezda BAGRETS (Karlsruhe Institute of Technology) Dr. Andrea CORNACCHINI (CERN EN Dept.) Mr. Miguel FERNANDES (CERN BE.
Harold G. Kirk Brookhaven National Laboratory High-Field Solenoids for a MC Final Cooling System AAC 2012 Austin, Texas June 11-15, 2012.
Injection Energy Review D. Schulte. Introduction Will review the injection energy So could answer the following questions: Which injection energy can.
FET-OPEN proposal for a HTS fast cycled magnet for Energy Efficiency and Operational Flexibility Motivations SC magnets are the choice of reference to.
Dipole design at the 16 T frontier - Magnet R&D for a Future Circular Collider (FCC) at Fermilab Alexander Zlobin Fermilab.
BNL High Field and HTS Magnet Program Ramesh Gupta BNL, NY USA H T.
CERN Accelerator School Superconductivity for Accelerators Case study 3 Paolo Ferracin ( ) European Organization for Nuclear Research.
JRA on Development of High Temperature SC Link Motivation Work Packages Partners & resources Amalia Ballarino Esgard open meeting CERN,
US-side contributions to the EUCARD2 collaboration Planning video meeting May 16, 2013.
Superior performance. powerful technology. SuperPower Inc. is a subsidiary of Furukawa Electric Co. Ltd. SuperPower 2G HTS Conductor Drew W Hazelton Director.
EuCARD-2 is co-funded by the partners and the European Commission under Capacities 7th Framework Programme, Grant Agreement WP10- Future Magnets.
Los Alamos National Laboratory Operated by the University of California for the U.S. Department of Energy “Development of High Temperature Superconductor.
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.
Muons, Inc. 14 Jan 2010 S. Kahn--IR Quads 1 IR Quadrupoles with Exotic Materials Steve Kahn, Muons Inc. Bob Palmer, BNL Don Summers, Ole Miss.
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.
Soumen Kar 1,2, Xiao-Fen Li 1, Venkat Selvamanickam 1, V. V. Rao 2 1 Department of Mechanical Engineering and Texas Center for Superconductivity University.
Concept of in-situ repair using laser based additive manufacturing techniques Prof. Toms TORIMS Riga Technical University, Latvia FCC Week 2016, Rome.
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,
New Magnet Technology (for high field) Lucio Rossi CERN INFN - CNS1 future strategy Elba 22 May 2014.
Conductor on Round Core (CORC) cables for power transmission and high-field magnets Danko van der Laan MAP HTS Magnet Workshop, Fermilab, May 31 st 2012.
Conductor Requirements for Magnet Designers DOE- Conductor Development Program Daniel R. Dietderich Superconducting Magnet Program Office of Science ICFA.
Lucio Rossi The High Luminosity LHC Project Distinguished Lecturer 2013.
The FCC Magnet Program seen from CERN Meeting at ASC-2014, Charlotte, August 13t, 2014.
CORC®: Results and Perspectives Danko van der Laan and Jeremy Weiss
2012 Applied Superconductivity Conference, Portland, Oregon
Yutaka Yamada (SIT, IEA-HTS OA)
Development of Nb3Sn (and Bi-2212) strands in preparation for the FCC
CERN Conductor and Cable Development for the 11T Dipole
Naoyuki Amemiya Kyoto University
To be presented at Nb3Al R&D Review,
CHEN, Fusan KANG, Wen November 5, 2017
DESIGN OPTIONS IN THE T RANGE
EuCARD2 WP 10.2 HTS Conductor
Preliminary study of HTS option for CEPC detector magnet
Muon Collider Magnet Technologies/Challenges
Muon Collider SR and IR Magnets
Qingjin XU Institute of High Energy Physics (IHEP),
Presentation transcript:

Report from WAMHTS-1 in Hamburg @ EuCARD2 CM Lucio Rossi With contribution from L. Bottura and L. Cooley and other participants

WAM HTS – 1 General Triggered by HE-LHC, alter FCC-hh EuCARD2 Following tradition of WAMS and WAMSD, it has been the 1st dedicated to HTS technology for Accelerator Magnets. Aim was to provide a forum where material scientists, conductor designers, and magnet engineers, all meet, also with Industry. 57 participants in WAMHTS-1 in Hamburg 12/11/2014 L Rossi @ WAMHTS-2 Kyoto

The FCC-hh is the main goal (but not the only one ) 100 km, 16 T 100 TeV (c.o.m.) FCC-hh 80 km, 20 T 100 TeV (c.o.m.) Geneva PS HE-LHC 27 km, 20 T 33 TeV (c.o.m.) SPS LHC L. Bottura at WAMHTS-1 LHC 27 km, 8.33 T 14 TeV (c.o.m.) 12/11/2014 L Rossi @ WAMHTS-2 Kyoto

A summary HTS for field (MB) HTS for operating margin (D1) Attain o(20) T, reducing length and civil engineering in the main dipoles, and providing ad-hoc solutions for specific regions (e.g. function similar to the LHC 11 T Nb3Sn dipole). Only HTS can do this HTS for operating margin (D1) The FCC IR and collimator regions will be a “hell of a place”, with particles and energies never experienced before. Radiation tolerance, heat removal and temperature margin will be paramount to reliable operation. HTS can do this HTS for low consumption (booster/injector) The FCC injector complex requires high energy efficiency to maintain the installed power at a reasonable level (e.g. the LHC SPS uses today o(50) MW). HTS at 20…77 K is a good candidate for this HTS for power transmission The scale of the accelerator requires high-current lines over km lengths. HTS, combined with advances in cryogenic distribution, would be the ideal solution 12/11/2014 L Rossi @ WAMHTS-2 Kyoto

HEP & HTS HEP has never been a driver for HTS Since a few years it is WAMHTS-1 hs enhanced this positive dynamism Stared in USA af ew years ago Boosted by HE-LHC and FCC Other projects in Japan and elsewhere Company are looking at us with interest 8 superconductor companies attended WAMHTS-1 !! We need not deceive them 12/11/2014 L Rossi @ WAMHTS-2 Kyoto

Results of the HEP - HTS Return of interest toward High Field (say > 10 T) Low temperature 4-20 K regime For us they are not HTS : they are HFS High Field Superconductors Now many reputed companies (except one) have optimization program for high field; laboratories are studying how to relate characterizion at 77 K s.f. (easy and continuous) to properties at 4.2 K – 20 T This interest  indicator of difficulties in penetrating the real marked for us economics is important but not a barrier – to a certain extend We are a good partner, willing to test with perseverance 12/11/2014 L Rossi @ WAMHTS-2 Kyoto

Compilation producers by Lance Cooley and Luca Bottura Region Vendor Material and Route* E.U. Bruker (internal use) REBCO (ABAD+PLD)   SuperOx REBCO (IBAD+PLD) Theva (not attending) YBCO (ISD+RCE) U.S.A. SuperPower YBCO (IBAD+MOD) AmSC (internal; not attending) REBCO (RABiTS+MOD) Asia Fujikura (also Europe) Sunam REBCO (IBAD+RCE/DR) Sumitomo DI Bi-2223 There are more HTS producer than Nb-Ti ! To add : OST for Bi-2212 (in other session) * REBCO = rare-earth (usually Gd) doped YBCO, where YBCO = YBa2Cu3O7-x; IBAD/ABAD = Hastelloy C or stainless steel substrate with MgO buffer layer textured by ion/alternating beam assisted deposition; PLD = pulsed laser deposition; RCE = reactive combination of elements; ISD = inclined substrate deposition; MOD = metal-organic chemical vapor deposition; RABiTS = rolling assisted bi-axial textured substrates; DR = diffusion reaction. 12/11/2014 L Rossi @ WAMHTS-2 Kyoto

Recommendation following tape session Unification of terminology : lift factor… (ratio between performance at different temperature – field…) Increasing the YBCO thickness is a direct route for increasing the overall current density. Process optimization should maintain or improve the critical current variation along the unit length to 2.5%. Batch-to-batch consistency of critical current should be maintained at 5% level among unit lengths. Kilometer unit lengths should be achieved. Conductor thickness should be controlled to better than 5 mm, and width to better than 50 mm, including copper coating, to avoid stress concentration during winding or cabling. 12/11/2014 L Rossi @ WAMHTS-2 Kyoto

Conductor CORC is certainly making competition to Roeble Other configuration (stacked tape) are also considered, with different problem We do not have an ideal cable – conductor - today… Je tape is now not far for our goal! Need UNIFORMITY and long lengths & cost reduction How to transform the good tape perfomance int a good conductor? Except Bi-2212: Rutherford cable is a gift However the 1 producer; the overpressure in O2 atmosphere and the transverse pressure needs to be addressed and demonstrated to be not a practical show- stopper 12/11/2014 L Rossi @ WAMHTS-2 Kyoto

Points of reflection (provocations) to Magnet Designer and Engineers Industry needs orders… Industy need continuous orders… The downselection today is too early: we do not not know which of the variou processes will be the best for industrial production HTS Conductor is not yet mature to make good magnets Magnet manufatcurer must use the HTS as it is now Built devices that reach a single goal (single goal demo, rather than final demo) even if the whole set of parameters for the application is not met, yet Are we ready to use a conductor not good enough? HTS means HIGHER STABILITY, evn at 4.2 K: how we use this characteristic? Are we ready to rediscuss margins and other categories? Mantras are not good for accommodate novelties 12/11/2014 L Rossi @ WAMHTS-2 Kyoto