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Quench Simulation at GSI

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laird
23 diapositives · 453 Views · Aug 29, 2014

Quench Simulation at GSI. FAIR Project. Quench. A sudden transition from the superconducting state to the normal-conducting state. Quench causes: conductor movement eddy currents in the conductor beam losses poor cooling. Self-protecting and not self protecting magnets.

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  1. Quench Simulation at GSI August 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 1

  2. FAIR Project June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 2

  3. Quench • A sudden transition from the superconducting state to the normal-conducting state. • Quench causes: • conductor movement • eddy currents in the conductor • beam losses • poor cooling June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 3

  4. Self-protecting and not self protecting magnets If max. temp. < 300 (350) K and max. voltages (coil-to-ground, coil-to-coil) do not damage the insulation magnet / group of magnets is self protecting if not Quench protection is required dump resistors, cold diodes, quench heaters etc. June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 4

  5. Self-protecting and not self protecting magnets:Tau and MIITs June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 5

  6. Self-protecting and not self protecting magnets@ FAIR • All Super-FRS magnets - self protecting • SIS100 rings (dipole ring, quadrupoles rings, chromaticity sextupoles - 6 magnets in series, other correctors) – not self-protecting • single SIS100 dipole almost self-protecting • SIS300 magnets – not self-protecting June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 6

  7. FAIR Project: Super-FRS Super-FRS dipole (66 um) Potted coil: 28 layers, 20 turns/layer In= 232 A, Emag=414 kJ DC machine 3D Simulation June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 7

  8. FAIR Project: SIS100 Nuclotron cable SIS100 dipole (2 layer prototype, 4.3 um) June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 8

  9. FAIR Project: SIS100 dipole magnetsfast cycling 2 T/s -> 28 kA/s, one dipole = 47 kJ 1D Simulation Insulated wire and 23 wires + CuNi tube FoS dipole magnet 109 dipoles in series 13.1 kA, 1.9 T, CuMn matrix in order to reduce AC losses June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 9

  10. FAIR Project: SIS100 quadrupole magnets 1D Simulation Insulated wire and 23 wires + CuNi tube up to 84 quadrupoles in series 3 quadrupole circuits: QD, F1 and F2 June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 10

  11. FAIR Project: SIS100 corrector magnets • Chromaticity sextupole magnets • Steering magnets (2 dipoles) • Multipole corrector magnets (Quadrupole + Sextupole + Octupole) 1D Simulation Insulated wire June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 11

  12. TEVATRON FAIR Project: SIS300 Rutherford cable ArjanVerweij’s talk June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 12

  13. FAIR Project: other superconducting magnets • High Energy Beam Transfer Line (HEBT) • SIS300 type magnets (Rutherford cable), line to CBM and beam dump • CBM Dipole • potted coil, “wire in channel”, similar to Super-FRS, 5.15 MJ • Quadrupoles of HEDgeHOB final focusing system (Rutherford cable) June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 13

  14. GSI Quench Program @ microscopic scale @ macroscopic scale June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 14

  15. Heat-balance equation (implicit method) i – position j – time June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 15

  16. GSI Quench Program Equation matrix Initial temperature profile is known! i – position j – time we compute: then electrical equation is updated to avoid high jumps in temperature, an adaptive time stepping algorithm is applied (max dT is fixed) June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 16

  17. 3D Simulation vs. measurements Super-FRS dipole (prototype) June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 17

  18. 3D Simulation vs. measurements Super-FRS dipole (prototype) June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 18

  19. 3D Simulation vs. measurements Super-FRS dipole (prototype) June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 19

  20. 1D Simulation vs. measurements:SIS100 FoS dipole and 2 layer prototype 2 layer prototype FoS dipole June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 20

  21. Conclusion • One need to perform at least simplified quench calculation before the experiment. • Expected max. temp. and max voltages (coil-to-ground and coil-to-coil) need to be known in advance safety of the machine and personnel! • Tmax < 300 (350) K, sometimes lower < 100 K; High Voltage (HV)! Insulation? Electrical sockets? • HV? He gas in the cryostat? Paschen effect! • Small change in MIITs value • corresponds in a big change in Tmax. • Quench calculation is a part of the machine design! June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 21

  22. Thank you for attention! June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 22

  23. Quench Detection June 18th 2014 | TEMF TU Darmstadt / GSI | Piotr Szwangruber | 23