Stellarator magnet options. Electrical/winding issues Elegant solution for ARIES-AT does not extrapolate well for ARIES-CS –High Temperature Superconductor.

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

Q1 for JLAB’s 12 Gev/c Super High Momentum Spectrometer S.R. Lassiter, P.B. Brindza, M. J. Fowler, S.R. Milward, P. Penfold, R. Locke Q1 SHMS HMS Q2 Q3.
3nd KEK-CEA Workshop on Superconducting magnets and cryogenics for accelerator frontier - 24/03/2009 Ceramic insulation for Nb3Sn accelerator magnets F.Rondeaux.
Fessia Paolo, David Smekens and the whole TE-MSC-MDT section Insulation strategies and materials for incoming SC magnets.
Undulator R & D Jim Clarke STFC Daresbury Laboratory, UK BAW-2 SLAC Jan 2011.
Physics and Technology Trade-Offs in Optimizing Compact Stellarators as Power Plants Farrokh Najmabadi and the ARIES Team UC San Diego 21 st IEEE Symposium.
Preliminary Analysis of the Target System Magnets 1.Version with a 6-T copper magnet insert 2.Version with a 6-T high-temperature superconductor insert.
Magnet System Definition L. Bromberg P. Titus MIT Plasma Science and Fusion Center ARIES meeting November 4-5, 2004.
1 The Genoa Tracker Solenoids and their Contribution toward a New Design Michael A. Green Lawrence Berkeley National Laboratory and Pasquale Fabbricatore.
Overview of ARIES Compact Stellarator Study Farrokh Najmabadi and the ARIES Team UC San Diego US/Japan Workshop on Power Plant Studies & Related Advanced.
ARIES-Stellerator studies Magnet issues L. Bromberg P. Titus MIT Plasma Science and Fusion Center Cambridge MA May 7, 2003.
Superconducting Solenoids for COMET KEK Cryogenics Center, Osaka Univ. Kuno-san’s Team, J-PARC MLF Muon Group.
Overview of the ARIES-CS Compact Stellarator Power Plant Study Farrokh Najmabadi and the ARIES Team UC San Diego Japan-US Workshop on Fusion Power Plants.
HTS Magnets for ARIES-AT L. Bromberg J.H. Schultz MIT Plasma Science and Fusion Center ARIES Meeting March 20, 2000.
Stellarator magnets L. Bromberg J.H. Schultz MIT Plasma Science and Fusion Center ARIES meeting March 8-9, 2004.
CM-18 June Magnet Conductor Parameters and How They affect Conductor Selection for MICE Magnets Michael Green Lawrence Berkeley Laboratory Berkeley.
Twin Solenoid Twin Solenoid - conceptual design for FCC-hh detector magnet - Matthias GT Mentink Alexey Dudarev Helder Pais Da Silva Leonardo Erik Gerritse.
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.
Magnet Options for Modular Stellarator Power Plants Leslie Bromberg J.H. Schultz ARIES team MIT Plasma Science and Fusion Center Cambridge MA US/Japan.
Magnet considerations for ARIES IFE L. Bromberg With contributions from J.H. Schultz MIT Plasma Science and Fusion Center ARIES Meeting Madison, WI September.
Magnet considerations for ARIES IFE HTS/LTS algorithms and design options L. Bromberg With contributions from J.H. Schultz MIT Plasma Science and Fusion.
Aug 29, 2006S. Kahn T HTS Solenoid1 A Proposal for a 50 T HTS Solenoid Steve Kahn Muons Inc. August 29, 2006.
Magnet costs L. Bromberg J.H. Schultz ARIES Meeting & Review PPPL, October
Superconducting Large Bore Sextupole for ILC
Muons, Inc. AAC Feb. 4, 2009 V. Kashikhin 1 Fermilab AAC  V. Kashikhin for Superconducting Magnet Team Superconducting Helical Solenoids.
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.
1 A Joint Proposal for US-Japan Cooperation Program Proposal to JSPS US-Japan collaboration fund R&D of superconducting magnet technology for high intensity.
Davide Tommasini Nb3Sn versus NbTi in HeII THERMOMAG-07, Paris 19 November 2007 Typical insulations for Rutherford cables Heat transfer model Heat flux.
Possible HTS wire implementation Amalia Ballarino Care HHH Working Meeting LHC beam-beam effects and beam-beam interaction CERN, 28 th August 2008.
Status of CEPC Detector magnet
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.
Some considerations and back-of-the-envelope computations on the multipole correctors Giovanni Volpini, CERN, 7 March 2013.
11 T Nb3Sn Demonstrator Dipole R&D Strategy and Status
S. Caspi, LBNL HQ Progress and Schedule Shlomo Caspi LBNL LARP Collaboration Meeting – CM13 Port Jefferson November 4-6, 2009.
Review of Quench Limits FermilabAccelerator Physics Center Nikolai Mokhov Fermilab 1 st HiLumi LHC / LARP Collaboration Meeting CERN November 16-18, 2011.
E. Todesco PROTECTION IN MAGNET DESIGN E. Todesco CERN, Geneva Switzerland With help from B. Auchmann, L. Bottura, H. Felice, J. Fleiter, T. Salmi, M.
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.
Magnet for ARIES-CS Magnet protection Cooling of magnet structure L. Bromberg J.H. Schultz MIT Plasma Science and Fusion Center ARIES meeting UCSD January.
Superconducting Magnet Group Superconducting magnet development for ex-situ NMR LDRD 2003 Paolo Ferracin, Scott Bartlett 03/31/2003.
WAMSDO-2013, New Techniques, GdR WAMSDO, January 2013 Gijs de Rijk CERN 1 NEW TECHNIQUES.
BNL High Field and HTS Magnet Program Ramesh Gupta BNL, NY USA H T.
Undulator Insulation materials Simon Canfer Advanced Materials Group Applied Science Division Technology
CERN Accelerator School Superconductivity for Accelerators Case study 3 Paolo Ferracin ( ) European Organization for Nuclear Research.
1 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September 2004 PIONEERING SUPERCONDUCTING MAGNETS IN LARGE TOKAMAKS.
FRESCA2 Technical Meeting 5-Validation of coil winding with Cu coils Françoise Rondeaux 09/06/ CEA-Irfu-SACM-LEAS - 5-Rondeaux- FRESCA2 Technical.
Task 6: Short Period Nb3Sn Superconducting Helical Undulator George Ellwood
E. Todesco, Milano Bicocca January-February 2016 Appendix C: A digression on costs and applications in superconductivity Ezio Todesco European Organization.
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.
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,
D. Arbelaez for the LBNL LCLS SCU team Mar. 3,
J. Polinski, B. Baudouy -The NED heat transfer program at CEA CEA Saclay, January 11th NED heat transfer program at CEA NED heat transfer program.
Answers to the review committee G. Ambrosio, B.Bordini, P. Ferracin MQXF Conductor Review November 5-6, 2014 CERN.
2 nd LARP / HiLumi Collaboration Mtg, May 9, 2012LHQ Goals and Status – G. Ambrosio 11 Quench Protection of Long Nb 3 Sn Quads Giorgio Ambrosio Fermilab.
FNAL Workshop, July 19, 2007 ILC Main Linac Superconducting Quadrupole V.Kashikhin 1 ILC Main Linac Superconducting Quadrupole (ILC HGQ1) V. Kashikhin.
The most likely cause of death for a superconducting magnet Input data for thermal modeling of Nb 3 Sn Superconducting Magnets by Andrew Davies Find the.
CHATS-AS 2011clam1 Integrated analysis of quench propagation in a system of magnetically coupled solenoids CHATS-AS 2011 Claudio Marinucci, Luca Bottura,
Superconducting Coils for Application
A model superconducting helical undulators wound of wind and react MgB2 and Nb3Sn multifilamentary wires Center for Superconducting & Magnetic Materials.
Superconducting magnet
HO correctors update Massimo Sorbi and Marco Statera
Quench estimations of the CBM magnet
WP-7 / Task 4 Very high field magnet
Superconducting Helical Solenoids
Q0 magnet, cooling, support ideas
HTS Magnet R&D at BNL Ramesh Gupta November 17, 2017.
To be presented at Nb3Al R&D Review,
CEA Nb3Sn quadrupole magnet : test results and future
Quench calculations of the CBM magnet
Review of Quench Limits
Presentation transcript:

Stellarator magnet options

Electrical/winding issues Elegant solution for ARIES-AT does not extrapolate well for ARIES-CS –High Temperature Superconductor epitaxially deposited on structure –Magnet protection for HTS magnets very difficult because of very low speed of propagation of quench Very good mechanical and thermal contact between HTS and structure makes quench energetically impossible (very high temperature/energy margins) Instead ARIES CS magnet wound in structural semi-continuous cases

Winding for ARIES-CS Need ductile conductor because of strains required during winding process Options: –NbTi-like SC Helias Stellarator design uses NbTi at reduced temperature (2K) Problem with temperature margin –Wind and react Nb 3 SN or MgB 2 Need to maintain structural integrity during heat treatment (700 C for a few hundred hours) No organic material, difficult to use glass.

Low temperature SC winding pack current density

Issues that need to be addressed for Wind-and-React magnets Minimization of the conductor size –Ease the winding process Inorganic insulation, assembled with magnet prior to winding and thus capable to withstand the Nb 3 Sn heat treatment process. –Two groups (one in the US, the other one in Europe) have developed glass-tape that can withstand the process –The US process uses organic resin/epoxy after heat treatment –The EU process uses all inorganic process

EU process tape (clay/glass, with glass tapes) A. Puigsegur et al., Development Of An Innovative Insulation For Nb3sn Wind And React Coils

The dielectric strength at 4.2 K is ~ 75 kV/mm –similar to traditional insulations with vacuum- impregnated of epoxy resin

Quench protection To minimize size of conductor for winding, minimize copper in conductor –J Cu ~ 200 A/mm 2 (200 MA/m 2 ) –Magnet dump < 4 s, preferable ~ 2 s (150 K) –50 GJ stored energy –20 kV maximum voltage (0.5 mm thick insulation) –2 dump circuits per coil –Conductor current ~ 40 kA –Conductor size ~ 3.5 cm 2 –Substantially smaller than ITER conductor –Can it be wound inside case?

Consistency Magnet design –Use Nb 3 Sn, wind and react –Use 0.5 mm inorganic insulation w/o organic resin/epoxy (20 kV max voltage) –Use 40 kA winding pack current –Use 2 dump-circuits per coil (~50 pairs of current leads) –0.1 W/kA, ~500 W cooling Not pretty, but self-consistent Need to provide costing to system code

Future work Work with UCSD and ORNL for a better definition of the coil structure –Coil looks wimpy in the outside, very thick in the inside –Bucking vs wedging Heat loads to coil Transfer of loads to warm support