1 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September 2004 PIONEERING SUPERCONDUCTING MAGNETS IN LARGE TOKAMAKS.

Slides:



Advertisements
Similar presentations
Inspection & Preventive maintenance of breakers
Advertisements

MQXF Quench Protection Analysis HiLumi workshop – KEK, Tsukuba Vittorio Marinozzi 11/18/2014.
MUTAC Review, 9 April MuCOOL and MICE Coupling Magnet Status Michael A. Green Lawrence Berkeley Laboratory Berkeley CA
F.Millet - Preparation Meeting for the FCC International Collaboration BoardSeptember 9, / 5 CEA-Grenoble Contribution New challenges for the FCC.
Unit 19 Measurements of strain, stress, and coil mechanical properties
CASIPP Design of Cryogenic Distribution System for CFETR CS model coil Division of Cryogenic Engineering and Technical Institute of Plasma Physics Chinese.
1/10CCFW 34, Garching, June 24th TORE SUPRA Association Euratom-Cea S. BRÉMOND A few very simple technical elements on the internal / external matching.
Construction of Wendelstein 7-X Max-Planck-Institut für Plasmaphysik
CRYOGENICS AND POWERING
Status of CEPC Detector magnet
SOFT 2004 OVERVIEW OF CRYOGENIC TECHNOLOGY FOR THE THERMONUCLEAR FUSION P. DAUGUET, M. BONNETON, P. BRIEND, F. DELCAYRE, B. HILBERT, A. RAVEX Air Liquide.
Workshop on Beam losses, heat deposition and quench levels for LHC magnets, Geneva, 3-4 March 2005 Liquid helium heat transfer in superconducting cable.
1 Cryogenic in Fusion Devices” Kavita Rathore MTech – NST Delhi University.
The cryogenic systems of the ATLAS and CMS detectors Johan Bremer on behalf of TE/CRG 06/06/2013AFF.
Accelerators for ADS March 2014 CERN Approach for a reliable cryogenic system T. Junquera (ACS) *Work supported by the EU, FP7 MAX contract number.
Overview of the KSTAR commissioning M. Kwon 3 June, 2008.
Workshop on Beam Induced Quenches Summary of session 4 “Heat Transfer R&D” SpeakersTopics Pier Paolo Granieri Steady-State Heat Transfer in the LHC Superconducting.
1 Second LHC Splice Review Copper Stabilizer Continuity Measurement possible QC tool for consolidated splices H. Thiesen 28 November 2011 K. Brodzinski,
/18 Cryogenic thermometry for refrigerant distribution system of JT-60SA Kyohei NATSUME, Haruyuki MURAKAMI, Kaname KIZU, Kiyoshi YOSHIDA, Yoshihiko KOIDE.
Thermal and electrical analysis of superconducting magnets Some available tools and results L. Bottura Review on the Thermal Stability of Superconducting.
Superconducting IR Magnets CHEN, Fusan May 11, 2007.
Artificial Neural Networks (ANN) modeling of the pulsed heat load during ITER CS magnet operation L. Savoldi Richard 1, R. Bonifetto 1, S. Carli 1, A.
Thermal and flow processes in cryogenic systems following failure modes combined with superconducting magnets resistive transitions. M. Chorowski, M. Grabowski,
WAMSDO-2013, New Techniques, GdR WAMSDO, January 2013 Gijs de Rijk CERN 1 NEW TECHNIQUES.
Magnet design issues & concepts for the new injector P.Fabbricatore INFN-Genova Magnet design issues & concepts for the new injector P.Fabbricatore INFN-Genova,
Stellarator magnet options. Electrical/winding issues Elegant solution for ARIES-AT does not extrapolate well for ARIES-CS –High Temperature Superconductor.
JRA on Development of High Temperature SC Link Motivation Work Packages Partners & resources Amalia Ballarino Esgard open meeting CERN,
Luigi Serio CRYOGENICS PERFORMANCE AND OPERATION L. Serio, on behalf of the LHC Cryogenics Operation and Cryogenics Performance Panel.
Heat loads and cryogenics L.Tavian, D. Delikaris CERN, Cryogenics Group, Technology Department Accelerators & Technology Sector Friday, October 15, 20101HE-LHC'10.
11 T Dipole Project CERN Status M. Karppinen 11 T Management meeting 1 July 2013.
Cryogenic Summary - K. C. Wu Testing D2L102 in MAGCOOLJune, 02 Difference between D2L102 and D2L101 Operating Summary Cooldown to 100 K and 6 K Test Condition.
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,
Powering the damping rings wigglers Daniel Siemaszko, Serge Pittet OUTLINE : Powering superconductive magnets, Powering wigglers strategy, Existing.
Super Fragment Separator (Super-FRS) Machine and Magnets H. Leibrock, GSI Darmstadt Review on Cryogenics, February 27th, 2012, GSI Darmstadt.
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,
XVII SuperB Workshop and Kick Off Meeting - La Biodola (Isola d'Elba) Italy May 28 th June 2 nd 2011 P.Fabbricatore Sezione di Genova The air core magnets.
KEK-CEA Superconducting Magnet Co-operation Program The FJPPL workshop LAPP, Annecy-Le-Vieux (France), June LHC-3 Superconducting Magnets.
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.
Shrikant_Pattalwar ICEC 26, March 7-11, 2016, Delhi 1 Horizontal Tests in a Vertical Cryostat Shrikant Pattalwar STFC Daresbury Laboratory UK.
Sextupole Single Coil Test Results Giovanni Volpini on behalf of the LASA Team Giovanni Volpini, CERN, 22 April 2015.
Magnetics Program Highlights VLT Conference Call September 13, 2000 presented by J.V. Minervini MIT Plasma Science and Fusion Center.
Answers to the review committee G. Ambrosio, B.Bordini, P. Ferracin MQXF Conductor Review November 5-6, 2014 CERN.
Superconducting Cryogen Free Splittable Quadrupole for Linear Accelerators Progress Report V. Kashikhin for the FNAL Superconducting Magnet Team (presented.
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.
Hot-Spot Temperature Experiment Chats Workshop 10 th October 2013 Kamil Sedlak, Pierluigi Bruzzone EPFL-CRPP, Villigen, Switzerland.
1 Young-Ju Lee Vacuum & Cryogenic Engineering Team National Fusion Research Institute Young-Ju Lee Vacuum & Cryogenic Engineering Team National Fusion.
Max-Planck-Institut für Plasmaphysik 1 ICEC 26- ICMC 2016 March 7-11, 2016, New Delhi, India Michael Nagel Cryogenic commissioning, cool down and first.
Cryogenic Heat loads Analysis from SST-1 Plasma Experiments N. Bairagi, V. L. Tanna and S. Pradhan SST-1 Mission Institute for Plasma Research, Bhat, Ganhinagar.
Introduction to W7-X Coil Testing at CEA – Saclay, France G.Croari – March 2008.
Jim Kerby Fermilab With many thanks to Vladimir Kashikhin, the FNAL, KEK, and Toshiba teams. SCRF BTR Split Quadrupole ILC ML & SCRF Baseline Technical.
SUPERCONDUCTING MAGNETIC ENERGY STORAGE SYSTEM
The Stekly criterion in question Why Cable in conduit conductors ?
Instrumentation for status monitoring of SST-1 superconducting magnets
Cryogenic Safety- HSE seminar CERN,
Study and Development of Large Cryogenic Systems in China
Final doublet: future activity plan
Hervé Allain, R. van Weelderen (CERN)
Cooling down of W7-X coils with/without casing circulation
Innovative He cycle Francois Millet.
The CMS magnet superconducting coil
EPFL-SPC, 5232 Villigen PSI, Switzerland
Experience: past events and accidents
Introduction to W7-X Coil Testing at CEA – Saclay, France
CRYOGENICS OPERATIONS 2008 Organized by CERN
Cooling aspects for Nb3Sn Inner Triplet quadrupoles and D1
High Magnetic Field Lab, CAS
Thermohydraulic behaviour of the cryogenic system
Other arguments to train two sectors to 7 TeV
Optical fiber based sensors for low temperature and superconductors
J. Fleiter, S. C. Hopkins, A. Ballarino
Presentation transcript:

1 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September 2004 PIONEERING SUPERCONDUCTING MAGNETS IN LARGE TOKAMAKS : EVALUATION AFTER 16 YEARS OF OPERATING EXPERIENCE IN TORE SUPRA P. Libeyre, J.-L. Duchateau, B. Gravil, D. Henry, J.Y. Journeaux, M. Tena, D. van Houtte Association EURATOM-CEA, CEA/DSM/DRFC CEA Cadarache (France)

2 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September 2004 The Tore Supra tokamak at CEA Cadarache

3 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Introduction 2. Status of the Tore Supra Toroidal Field (TF) system 3.Normal operation 4.Fast safety discharges 5.The cryogenic system 6.Can the magnet experience of Tore Supra be useful for ITER ? 7.Conclusion

4 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Introduction (1/4) The Tore Supra TF magnet during assembly

5 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Introduction (2/4) Tore Supra TF coil structure Supercritical helium (4.5 K) in thick casing channels Superfluid helium (1.8 K) in thin casing bare conductors in superfluid helium !

6 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Introduction (3/4)  one of the largest superconducting system in operation (600 MJ magnetic energy)  Relying on a refrigerator including for the first time industrial quantities of superfluid helium ( Claudet bath) The Tore Supra TF system is :  Operated daily close to nominal conditions (1250 A) since November Continuous toroidal field on the whole day

7 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Introduction (4/4) The path to steady- state operation Introduction of a new type of refrigeration for superconducting magnets on an industrial level : Thousands of litres in TS (1988) Hundreds of thousands litres in LHC (2007) ! the continuous toroidal field allows long duration plasma experiments to be performed The revolution of superfluid helium The Tore Supra TF system contribution J.L Duchateau et al. “Monitoring and controlling Tore Supra toroidal field system: status after a year of operating experience at nominal current“ 1991 IEEE Trans. On Magn

8 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Status of the Tore Supra TF system (1/3) coil manufacture and magnet assembly  all coils tested up to nominal current (1 400 A) at Saclay 1988start of operation  short circuit in BT17 during a fast safety discharge 1989replacement of BT17 by spare coil BT19 acceptance tests of TF coils up to 1450 A (9.3 T)  quench of BT13 during fast safety discharge (FSD)  limitation of operating current to 1250 A  temperature increase observed in BT13 during FSD 1995disparition of defect on BT13  no more temperature increase in BT13 during FSD 2002continuous data acquisition system

9 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Status of the Tore Supra TF system (2/3) Similar behaviour of BT13 compared to the other coils Green light for TF operation 1.87 K No more apparent defect on BT13 Temperature increase in coils during FSD (2003)

10 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September 2004 Coil Critical current at 1.8 K (except BT19) Operation point Critical point Large margin (2.4 K) reduced nominal Load line Coil Critical current at 4.2 K (except BT19) Safe operation of the TF magnet since 1989 at 1250 A, 8 T 2. Status of the Tore Supra TF system (3/3) BT19

11 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Normal operation (1/4) Tore Supra TF activity Since 1988 Since 1988 :  13 thermal cycles from room to LHe temperature  TF cycles  plasma discharges

12 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Normal operation (2/4) Winding-pack temperature during one day of operation Temperature increase at current ramping-up and down (0.06 K) Green light for TF operation 1.87 K

13 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Normal operation (3/4) Thick casing helium temperature during one day of operation Temperature increase linked to cleaning plasma discharges

14 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Normal operation (4/4) Temperature increase due to a disruption from 1.7 MA Plasma disruption Thick casing : K Winding-pack : K 18/09/03

15 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Fast Safety Discharges (1/3) FSD Largest voltage at terminals (320 V at 1400 A) Risk of short circuit (bare conductors) To be avoided ! thermal load on cryogenic system 2h30 to recover Since 1989 : 75 Fast Safety Discharges of the TF magnet (on 1090 TF cycles) FSDTF cycles

16 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Fast Safety Discharges (2/3) Origin of Fast Safety Discharges since 1994 No FSD due to a quench !

17 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Fast Safety Discharges (3/3) Remedies to Fast Safety Discharges  Increase of trigger delays on alarms as much as possible without affecting the protection of the coil in case of a real quench  Sensor conditioning to decrease sensitivity to electric interference Optimisation of the protection

18 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September The cryogenic system (1/2) Availability Manpower : 12 persons Electric power : 1.1 MW Cost : 0.5 M€/year (excluding staff and energy) 2003 : 97 % 2002 : 92% availability

19 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September The cryogenic system (2/2) The major tendencies of the cryoplant ageing  loss of electrical insulation of many temperature sensors located in the depth of the cryostats.  drift of adjustment of the electronic components dedicated to the magnetic bearings of the cold compressors. Preventive maintenance of compressor units Good availability of the refrigerator Nevertheless, ageing signs are visible :

20 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September 2004 TF systemTore SupraITER Magnetic energy0.6 GJ40 GJ SuperconductorNbTiNb 3 Sn Conductor typemonolithic bare conductor 2.8 mm x 5.6 mm Cable-in-conduit TFMC (40.7 mm Ø) Conductor current1.4 kA68 kA Discharge voltage0.5 kV10 kV Cooling systemSuperfluid helium bath Supercritical helium forced flow Cryogenic power1.1 MW~ 35 MW 6. Can the TF magnet experience of Tore Supra be useful for ITER ? (1/4)

21 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September 2004 NbTi, 1.8 K NbTi, 4.5 K Nb 3 Sn,TFMC -0.65%, 4.5 K Tore Supra ITER 6. Can the TF magnet experience of Tore Supra be useful for ITER ? (2/4) Operation of ITER TF at 11.8 T doesn’t allow NbTi to be used

22 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Can the TF magnet experience of Tore Supra be useful for ITER ? (3/4) Extrapolation of the operation of the TF magnet from Tore Supra to ITER is not straightforward Forced flow cooling Very high voltage monitoring Fast safety discharge Tore Supra : no quench ITER : quench of all coils

23 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Can the TF magnet experience of Tore Supra be useful for ITER ? (4/4) experience of the CEA magnet team in conductor and coil design 16 years of reliable plasma operation with a TF superconducting magnet Decision to build ITER is possible ITER magnet R&D programme Still to be done Experience in TS can help : Design of protection and monitoring system Impact on cryoplant Detailed magnet operation Impact on scenarios

24 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September Conclusion The Tore Supra tokamak is the first important meeting between Superconductivity and Plasma Physics. Superconducting magnets can be operated successfully with plasma physics on the long term  Continuous operation of the toroidal field simplifies plasma discharge preparation  No significant heat load is associated to long shots  Continuous operation limits fatigue degradation The Tore Supra TF magnet is a useful tool to prepare ITER construction and operation