journal article·2019-09-01Open access

Experiment and numerical analysis on temporal stability of a bitter-like HTS magnet excited by MPFM

Xi Yuan, Yinshun Wang, Yueyin Wang, Yukai Qiao, Changtao Kan, Wei Pi

AIP Advances· Volume 9· Issue 9

Abstract

A full high temperature superconducting (HTS) magnet can operate in persistent current mode (PCM), which has promising application in high magnetic field. A laboratory scale Bitter-like HTS magnet stacked by REBaCuO (RE: rare earth element) annular plates was proposed and it can operate in PCM without current lead and joint resistance. This study focuses on the temporal stability of the magnetic field generated by the magnet, which was energized by the multi-pulsed field magnetization (MPFM) method composed of a solenoid coil and pulsed triangular waveform current source and tested at 77 K (LN2 bath). The characteristics of the magnetic field in the magnet with various pulsed current amplitudes, durations and reversal excitation experiments were systematically researched. Moreover, the numerical simulation of the magnet energized with the pulsed current amplitude 3A was performed and the attenuation of the magnetic field in the magnet was discussed and analyzed.
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Research context

OpenAlex topics: Physics of Superconductivity and Magnetism · Superconducting Materials and Applications · Magnetic and transport properties of perovskites and related materials

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

State Key Laboratory for Alternate Electrical Power System with Renewable Energy Sources, North China Electric Power University , Beijing 102206, China

Funding

National Natural Science Foundation of China

References (31)

Show source-provided references
1. Rev. Sci. Instrum. · 1936 · 7 · 47910.1166/asl.2012.3951 ↗
2. Science & Technology Review · 2018 · 36 · 93
3. IEEE Trans. Magn. · 1996 · 32 · 250310.1109/20.511381 ↗
4. IEEE Trans. Magn. · 1994 · 30 · 219210.1109/20.305707 ↗
5. IEEE Trans. Magn. · 1996 · 32 · 254210.1109/20.511391 ↗
6. IEEE Trans. Appl. Supercond. · 2014 · 24 · 460241210.1109/tasc.2013.2287707 ↗
7. IEEE Trans. Appl. Supercond. · 2016 · 26 · 430080710.1109/tasc.2016.2517022 ↗
8. IEEE Trans. Appl. Supercond. · 2016 · 26 · 430260410.1109/tasc.2015.2509172 ↗
9. IEEE Trans. Appl. Supercond. · 2018 · 28 · 430020510.1109/tasc.2017.2780043 ↗
10. IEEE Trans. Appl. Supercond. · 2011 · 21 · 162810.1109/tasc.2010.2093115 ↗
11. IEEE Trans. Appl. Supercond. · 2017 · 27 · 4600806
12. J. Magn. · 2016 · 21 · 23910.4283/jmag.2016.21.2.239 ↗
13. IEEE Trans. Appl. Supercond. · 2016 · 26 · 060610410.1109/tasc.2016.2524519 ↗
14. IEEE Trans. Appl. Supercond. · 2016 · 26 · 050050510.1109/tasc.2016.2526605 ↗
15. IEEE Trans. Appl. Supercond. · 2016 · 26 · 820070510.1109/tasc.2016.2535379 ↗
16. AIP ADV · 2017 · 7 · 09521810.1063/1.4998230 ↗
17. Supercond. Sci. Technol. · 2017 · 30 · 09400210.1088/1361-6668/aa7a51 ↗
18. IEEE Trans. Appl. Supercond. · 2010 · 20 · 103710.1109/tasc.2010.2043832 ↗
19. IEEE Trans. Appl. Supercond. · 2012 · 22 · 430220410.1109/tasc.2011.2178969 ↗
20. IEEE Trans. Appl. Supercond. · 2014 · 24 · 430080510.1109/tasc.2013.2283226 ↗
21. Appl. Phys. Lett. · 2013 · 102 · 10260110.1063/1.4795016 ↗
22. Supercond. Sci. Technol. · 2018 · 31 · 09LT0110.1088/1361-6668/aad34c ↗
23. IEEE Trans. Appl. Supercond. · 2018 · 28 · 460300510.1109/tasc.2018.2791937 ↗
24. IEEE Trans. Appl. Supercond. · 2019 · 29 · 470040510.1109/tasc.2018.2883132 ↗
25. IEEE Trans. Appl. Supercond. · 2019 · 29 · 490050510.1109/tasc.2019.2891671 ↗
26. IEEE. Trans. Magn. · 2000 · 36 · 122610.1109/20.877661 ↗
27. IEEE Trans. Appl. Supercond. · 2001 · 11 · 262710.1109/77.920407 ↗
28. IEEE Trans. Appl. Supercond. · 2016 · 26 · 680030510.1109/tasc.2016.2518580 ↗
29. IEEE Trans. Appl. Supercond. · 2018 · 28 · 680080510.1109/tasc.2018.2801328 ↗
30. IEEE. Trans. Appl. Supercond. · 2005 · 15 · 1710.1109/tasc.2004.839774 ↗
31. IEEE. Trans. Appl. Supercond. · 2014 · 24 · 8200433