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Superconducting Solenoid Punch. Team Supercool Andy Lin Chris Kinney Naomi Kohen David Schoen. Superconducting Actuator. Zero resistance at low T Electrical actuator: Electrical E Mechanical E American Superconductor Goal: HTS solenoid punch. Why superconducting?.
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Superconducting Solenoid Punch Team Supercool Andy Lin Chris Kinney Naomi Kohen David Schoen
Superconducting Actuator • Zero resistance at low T • Electrical actuator:Electrical E Mechanical E • American Superconductor • Goal: HTS solenoid punch
Why superconducting? Low resistance Higher efficiency Higher current density Larger field Fewer turns Simple design and manufacturing
Superconductor Physics • Impenetrable by external magnetic fields (up to a point) • Type I & II Superconductors • Cooper Pairs
BSSCO 2223: Our Tape • Provided by American Superconductor • 4 mm (w) x 0.21mm (t) • Critical Current rating 85 – 108 A • Critical Temp (Tc) 110K • Currently 2 pieces; 4 and 50 m long
The Punch • Use solenoid for magnetic field • An iron core accelerates in the field • A strong field will produce a significant force.
Coil Dimensions • Inner Coil between 50 mm and 100 mm in diameter • Coil height approximately 75mm • Between 320 and 160 turns with 50 meters of wire
Materials Choice • PVC • Inexpensive • Machinable • Diamagnetic • Al • Inexpensive • Easily Machinable • Paramagnetic • Durable
Estimates Force (N) Displacement (m)
Estimates Force (N) Displacement (m)
Future Considerations • Running colder than 77K • Making a taller or shorter coil • Punch striking surface • Punch shape • Retraction Mechanism • Pulse (with capacitor)?
Tests • Obtain comparable copper solenoid • Magnetic field • Force • Energy density per mass
Calculating Force • For Loop • Force: • Magnetization of Iron: 334225 A/m