The development of persistent joints for MgB2-based conductors

Slides:



Advertisements
Similar presentations
Faradays Law of Induction A changing magnetic field induces an electric field. The induced electric field causes a current to flow in a conductor.
Advertisements

Magnesium Diboride Program Hyper Tech Research Inc. Mike Tomsic Magnesium Diboride Workshop April 2003 Research Partners: Ohio State University-LASM National.
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,
P.Fabbricatore Sezione di Genova Joint Belle II & SuperB Background Meeting SuperB IR details:magnets SUPERB IR DETAILS: SC MAGNETS P.Fabbricatore INFN.
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Stellarator magnets L. Bromberg J.H. Schultz MIT Plasma Science and Fusion Center ARIES meeting March 8-9, 2004.
III. Results and Discussion In scanning laser microscopy, the detected voltage signal  V(x,y) is given by where j b (x,y) is the local current density,
Physics 121 Practice Problem Solutions 11 Faraday’s Law of Induction
Department of Materials Science and Engineering The development of persistent joints for MgB 2 -based conductors D. Doll 2, J. Yue 2, C.J. Thong 2, M.A.
ILC Main Linac Superconducting Cryogen Free Splittable Quadrupole Progress Report V. Kashikhin for Superconducting Magnet Team.
Lecture 12 Current & Resistance (2)
Possible HTS wire implementation Amalia Ballarino Care HHH Working Meeting LHC beam-beam effects and beam-beam interaction CERN, 28 th August 2008.
LBNL Test Cryostat Preliminary Design Review Tuning – Field Correction Soren Prestemon, Diego Arbelaez, Heng Pan, Scott Myers, Taekyung Ki.
Spectrometer Solenoid: Plans to Fix Magnet 2 Steve Virostek Lawrence Berkeley National Lab Spectrometer Solenoid Review November 18, 2009.
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.
15 Th November 2006 CARE06 1 Nb 3 Sn conductor development in Europe for high field accelerator magnets L. Oberli Thierry Boutboul, Christian Scheuerlein,
CERN Accelerator School Superconductivity for Accelerators Case study 1 Paolo Ferracin ( ) European Organization for Nuclear Research.
SCU1 Vertical Test Results Matt Kasa 9/16/2014. Vertical Cryostat Assembly Coil Training Record the current decay and the terminal voltage across the.
Department of Materials Science and Engineering Effects of Core Type, Placement, and Width, on ICR of Nb 3 Sn Rutherford Cables E. W. Collings, M. D. Sumption,
Test Program and Results Guram Chlachidze for FNAL-CERN Collaboration September 26-27, 2012 Outline Test program Quench Performance Quench Protection Magnetic.
Influence of Twisting and Bending on the Jc and n-value of Multifilamentary MgB2 Strands Y. Yang 1,G. Li 1, M.D. Susner 2, M. Rindfleisch 3, M.Tomsic 3,
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.
E. Todesco, Milano Bicocca January-February 2016 Appendix C: A digression on costs and applications in superconductivity Ezio Todesco European Organization.
1 W.Ootani ICEPP, University of Tokyo MEG experiment review meeting Feb , PSI W.Ootani ICEPP, University of Tokyo MEG experiment review meeting.
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.
Superconducting Cryogen Free Splittable Quadrupole for Linear Accelerators Progress Report V. Kashikhin for the FNAL Superconducting Magnet Team (presented.
CHATS-AS 2011clam1 Integrated analysis of quench propagation in a system of magnetically coupled solenoids CHATS-AS 2011 Claudio Marinucci, Luca Bottura,
Prototyping of Superconducting Magnets for RAON ECR IS S. J. Choi Institute for Basic Science S. J. Choi Institute for Basic Science.
Jim Kerby Fermilab With many thanks to Vladimir Kashikhin, the FNAL, KEK, and Toshiba teams. SCRF BTR Split Quadrupole ILC ML & SCRF Baseline Technical.
Results from the cold test of the first QD0 prototype
J.Yue, D. Doll, X. Peng, M.Rindfleisch, Mike Tomsic
C.J. Kovacs M.D. Sumption E.W. Collings
Superconducting Coils for Application
FEL SCU development at APS/ANL
Dipole magnets A dipole magnet gives a constant B-field.
MQXC Nb-Ti 120mm 120T/m 2m models
A model superconducting helical undulators wound of wind and react MgB2 and Nb3Sn multifilamentary wires Center for Superconducting & Magnetic Materials.
Milan Majoros, Chris Kovacs, G. Li, Mike Sumption, and E.W. Collings
2012 Applied Superconductivity Conference, Portland, Oregon
G.Z. Li Y. Yang M.A. Susner M.D. Sumption E.W. Collings
HO correctors update Massimo Sorbi and Marco Statera
Quench estimations of the CBM magnet
Status of the CLIC DR wiggler design and production at BINP
Magnetization, AC Loss, and Quench in YBCO Cables”
When we generate power we ramp up the voltage for transmission (up to V) and then when it arrives at homes we ramp it back down for convenient use.
Yury Ivanyushenkov for the UK heLiCal Collaboration
C. J. Kovacs, M. Majoros, M. D. Sumption, E. Collings
Challenges of vacuum chambers with adjustable gap for SC undulators
CERN Conductor and Cable Development for the 11T Dipole
M.D. Sumption, C. Myers, F. Wan, M. Majoros, E.W. Collings
Mike Sumption, M. Majoros, C. Myers, and E.W. Collings
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
HO Corrector Magnets: decapole test and future plans
Yingshun Zhu Accelerator Center, Magnet Group
Challenges for FCC-ee MDI mechanical design
X. Xu M. D. Sumption C. J. Kovacs E. W. Collings
Technical Summary - ANL
Measurements (to be made): About the device (in development):
CERN Accelerator School Superconductivity for Accelerators Case study 2 Paolo Ferracin European Organization for Nuclear Research.
X. Xu M. D. Sumption C. J. Kovacs E. W. Collings
C.J. Kovacs M.D. Sumption E.W. Collings M. Majoros X. Xu X. Peng
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Peter McIntyre Visit Overview Slides
Quench calculations of the CBM magnet
Chapter 28 Sources of Magnetic Field
Electron Collider Ring Magnets Preliminary Summary
Optical fiber based sensors for low temperature and superconductors
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:

The development of persistent joints for MgB2-based conductors M.D. Sumption, C. Kovacs, F. Wan, M. Majoros, E.W. Collings Center for Superconducting and Magnetic Materials, MSE, The Ohio State University D. Doll, C.J. Thong, D. Panik, M.A. Rindfleisch, M.J. Tomsic Hyper Tech Research Funded by an NIH bridge grant, and also an NIH NIH, National Institute of Biomedical Imaging and Bioengineering grant, under R01EB018363.

Outline Joint development – Hyper Tech is developing both superconducting solder type MgB2 persistent joints and MgB2-MgB2 persistent joints (for both W&R and R&W applications) OSU is developing the test process and performing the test of the MgB2 persistent joints First, direct I-V measurements are used which can probe down to R value of 10-10 ohms Results for the direct I-V probe are discussed Next, two decay rigs are described, capable of measuring R in the R= 10-12 and lower regime Then MgB2 joints reaching into the 10-12  regime are shown Finally, plans for persistent switch development, and coil segments with persistent joints/switches are described

Place of this effort in Larger goals Overall Goals Develop MgB2 joints which are ready for both W&R coils as well as R&W coils (R = 10-12-10-15 ) Develop persistent switch Integrate into sets of coil segments and test in OSU’s large cryocooled test cryostat Demonstrate an operating set of field coils with persistence for a whole body MRI (image guided system) Key step enabling commercial MRI applications

Test Sequence Demonstrate joints with R < 10-10  (measured by direct I-V). May be: (i) SC solder, R&W MgB2, W&R MgB2 Develop test rig and develop MgB2 joints with R = 10-12  and lower May be: W&R and R&W MgB2, multifilament, MRI-like strand

MgB2-MgB2 joint (example results) Screening test Simple I-V measurement Good to 10-10 

Summary of screening measurements of Persistent Joints Two styles of joints Superconducting solder type Direct MgB2-MgB2 In both cases, used already reacted wire Preliminary testing using direct I-V, R < 10-10  Next Step -- Decay Testing rig and samples for increased R sensitivity and decay test Working now to improve performance and measure to high sensitivity Superconducting Solder Type 4 K MgB2-MgB2Type 4 K

Persistent Joints Between Reacted MgB2 Wires MgB2 Wires Joined

Moving from screening test to decay test While further improvement in critical current of joints is still in process, it is important to measure R at values below 10-10  Thus, a decay rig was needed, as well as some initial testing and verification

Horizontal test arrangement for decay measurements – machine drawing MgB2 joint Hall probe inside, below gap level 100 A current leads NbTi primary coil SS holder assembly MgB2 secondary Gap in primary for secondary insertion NbTi primary coil

Actual Horizontal Test rig for decay measurements – with test NbTi joint mounted

NbTi/SC solder joint: test of Persistent joint apparatus Blue curve at right shows current in the NbTi primary. Red curve indicates the field reading by the Hall sensor. Protocol (by Regime): Use NbTi coil to generate Bcoil (I = 20 A) II. Increase the Bext to 3 T (pushes joint > SC) III. Drop Bext to 0. IV. Turn off NbTi coil rapidly. Note: Only the field in step IV indicates the field generated by the test (here NbTi) joint. Persistent regime, flat, very small decay

Expansion of decay region NbTi test joint Results for a NbTi persistent joint (at the time of stage III, IV in overview result). No interruption: current I primary was excited and de-excited, but no B field up and down ramp Field Interrupt: Field was cycled up and down while current was on Superconducting solder type. Shows initial time of 1 h run

Test of first persistent decay MgB2 sample Results for a MgB2 persistent joint (at the time of step III  IV along the lines of NbTi overview figure). Some trapping induced, but current decay is rapid Superconducting solder type.

Next Steps Test Device works Need to develop a lower R MgB2 joint In the meantime the MRI magnet design (image guided) wire becomes clear, optimizes with a larger wire Thus -- Need to test a joint made with a larger OD MgB2 wire Will need a modified holder which can handle larger OD wire

MRI Subscale and Fullscale wire Round wire OD = 0.95 mm 18 filament Outer Monel 32 % Cu SC = 12% Jc = 2 x 105 A/cm2, 5 T, 4 K Small MRI wire Ic = 155 A at 5 T, 4 K (0.95 mm OD) Large MRI wire Ic = 320 A at 5 T, 4 K Larger aspected wire Wire area = 1.46 mm2

Larger Strand, vertical Persistent Joint Test Assembly NbTi Primary Current injection Primary MgB2 secondary former Cu can MgB2 secondary Support rod Used large MRI wire for joint

MgB2 persistent joints under investigation Large diameter wire for demonstration magnet require new holder Investigating MgB2-MgB2 joint (not solder) Pursue first joint on unreacted wires (W&R style) Second joints on reacted wires (R&W style)

Step 1: Ramp external field, Bext up to reduce MgB2 Ic Protocol A: With Primary Step 2: Ramp up current in primary (Bext + Bp now present) Step 3: Ramp down external field, Bext to increase MgB2 Ic (at Bext = 0, Bp present) Step 4: Ramp down current in primary Secondary will attempt to retain Bp, observe decay with hall probe 40-turn NbTi Primary Primary Bp Ip Ip Bext 1.75-turn MgB2 Secondary Is Ips Secondary Bsec Hall-sensor centered in both primary and secondary SC-Joint

W&R Style- Zero Field Persistent joint results I Protocol Ramp to 4 T 50 A into Primary Ramp to zero field Turn off current Observe decay  is changing with time but reaches 3 x 105 sec R = 5 x 10-12 

Protocol B: Without Primary Step 1: Ramp external field, Bext up to reduce MgB2 Ic Step 2: Ramp down external field, Bext to increase MgB2 Ic and trap some of the previous Bext (at Bext = 0, Bext present) -- observe decay with hall probe. Baseline set by field in absence of joint Bext 1.75-turn MgB2 Secondary Is Ips Secondary Bsec Hall-sensor centered in both primary and secondary SC-Joint

Second run – zero field long time Protocol Ramp to 4 T Ramp to zero field Observe decay Tau = 3.7 x 105 sec R = 4 x 10-12 

W&R style Joint -- Persistent Current vs B Protocol Ramp to 4 T Ramp to zero field Observe decay B = 3 T  = 2.5 x 105 sec R = 3.8 x 10-11 

Next Steps R&W style joint Reduce R value even further – 10-15 , increase current performance and explore temperature performance Persistent Switch Coil segment (parallel development) Coil Segment Testing (basic operation, quench) Two Coil segment with SC joint and Persistent switch Demonstration of magnet system for image guided MRI system

Experimental Set up (2) Two stage GM cryocoolers (2) Cold heads attached to the copper ring Copper ring and coil are thermally connected with high purity copper strips 4 BSCCO leads for each current tap Heater attached in the copper ring to control the temperature of coil Data acquisition system: Nanovoltmeters (Keithley), Thermometers (Lakeshore), Data acquisition (Labview) Copper Ring MgB2 Coil Copper Strips

Layout for Demonstration coil and persistent switch

New Cro-conduction system Coils up to 1.5 m OD T down to 4 K 3 W at 4 K 700 A capacity

Summary Superconducting MgB2 joints are being developed, both W&R type and R&W type Initial screening results showed good results with R < 10-10 ohm, indicate that it was time to move to decay measurements The design of horizontal and vertical PJ decay rig were shown Direct MgB2-MgB2 joints using multifilamentary MgB2 of MRI-relevant design were demonstrated, with R in the 10-12  regime HTR/OSU are moving at an accelerated pace to develop useful MgB2 PJ, and are planning their test in a larger device Testing and development is in full swing, moving now to larger conductor joints for image guided system