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High Temperature Superconducting Solenoid Punch. Our Mission Make an actuator using BSSCO 2223 HTS tape from American Superconductor.

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Presentation on theme: "High Temperature Superconducting Solenoid Punch. Our Mission Make an actuator using BSSCO 2223 HTS tape from American Superconductor."— Presentation transcript:

1 High Temperature Superconducting Solenoid Punch

2 Our Mission Make an actuator using BSSCO 2223 HTS tape from American Superconductor

3 What is an actuator? MEMX High Performance Steerable MicroMirrors http://www.memx.com/products.htm A device that converts between mechanical energy and other forms Copper solenoids http://www.magnet-schultz.com/msafront2.jpg

4 Permanent magnet levitating over a superconductor http://helium.ee.tut.fi/supraryhma/images/korkealla.jpg What is a superconductor? A material that conducts without resistance A material that conducts without resistance Impenetrable by external magnetic fields (up to a point) Impenetrable by external magnetic fields (up to a point) Two types: Type I and Type II Two types: Type I and Type II Examples: Examples:  YBCO: Yttrium barium copper oxide  BSSCO 2212, 2223: (Bi,Pb) 2 Sr 2 Ca 1 Cu 2 O x, (Bi,Pb) 2 Sr 2 Ca 2 Cu 3 O x

5 BSSCO 2223 Structure BSSCO 2223 Unit Cell http://www.library.uow.edu.au/adt-NWU/uploads/approved/adt- NWU20030305.113225/public/02Whole.pdf

6 Our HTS Tape American Superconductor BSSCO 2223 4 mm (W) x 0.21 mm (T) Up to ~108 A Critical temperature (T C ) of 110 K

7 BSSCO 2223 Processing

8 BSSCO 2223: I C vs. H

9 Current vs. Bending Diameter

10 Actuator Choice Persistent actuator?  Can’t make superconducting junction Core choice  Magnetostrictive  Hard magnet  Soft magnet

11 Coil Radius Setup

12 Radius Measurements

13 The Apparatus

14 Field Calculations Magnetic field (tesla, cm)

15 Force Magnetization of Fe: 334225 A/m Force (N, cm)

16 Apparatus Fabrication

17 Solenoid Assembly

18 Assembled Solenoid

19 Testing: Magnetic Field

20 Testing: Magnetic Gradient 1 amp, room temperature

21 Self-Field Tests

22

23 Current Tests

24 Load Cell Setup

25 Force

26 Supercool

27 Conclusions Copper solenoid (1.5” x 2.4”) outperforms our actuator (force), even at room temperature

28 Energy Density Energy density of Supercool solenoid: 17400 J/m 3  7.0 cm outer diameter  3.36 J of total energy Energy density of 1.5” x 2.4” Cu solenoid: 16100 J/m 3

29 Further Considerations Commercial tape: > 135 A Colder temperature YBCO 2 nd generation tape  ~ 7 T at 77K

30 Acknowledgements Professor Chiang Professor Vander Sande Yin-Lin Xie David Bono Ken Stone Ed Moriarty Leslie Bromberg 3.082 staff

31 References YBCO second generation tape: http://www.amsuper.com/html/products/library/2g_white_paper_-_march_2004.pdf http://www.amsuper.com/html/products/library/2g_white_paper_-_march_2004.pdf Montgomery, D. Bruce. Solenoid Magnet Design: The Magnetic and Mechanical Aspects of Resistive and Superconducting Systems. Wiley-Interscience, New York. 1969. Magnet-Schultz commercial Cu solenoid: http://magnet-schultz.com/newRTP24X19INT.htm http://magnet-schultz.com/newRTP24X19INT.htm


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