AP-9-4

Design Methodology for High-Current Transformer-Rectifier Flux Pumps

15:30-15:45 30/11/2023

*James H.P. Rice1, Dominic A. Moseley1, Alexander Petrov2, Heng Zhang2, Steven Wray2, Rodney A. Badcock1
1. Paihau-Robinson Research Institute, Victoria University of Wellington, Lower Hutt 5010, New Zealand.
2. UK Atomic Energy Authority, Culham Science Centre, Abingdon OX14 3DB, United Kingdom.
Abstract Body

Flux pumps are DC superconducting power supplies capable of rapidly charging superconducting magnets to high currents[1,2]. Flux pumps using 2nd generation high-temperature superconductors (2G HTS) are rapidly progressing in development[3,4], but have yet to reach the high currents (>10 kA) of earlier low-temperature superconducting (LTS) flux pumps[5]. Increasing the current output of HTS flux pumps to >10 kA will show relevancy to high-current applications such as the toroidal field coils of next-generation fusion devices[6].

Here, we present the design methodology for HTS transformer-rectifier flux pumps. Using this methodology, devices of arbitrary current output can be rapidly developed and built. The basis of this is several studies on high-current transformer-rectifier components. These include: testing of HTS transformers using multi-wire, stacked-tape cable for secondary windings at 77 K; the asymmetry of critical current of single- or multi-wire switch elements using iron-core applied-field switches; and demonstration of a new method of operation for full-wave transformer-rectifier, capable of increasing experimental current output from 35 A to more than 275 A. Using this methodology, a preferred design for a 10 kA flux pump is presented.

References

[1] L. J. M. van de Klundert and H. H. J. ten Kate, “Fully superconducting rectifiers and fluxpumps Part 1: Realized methods for pumping flux,” Cryogenics, vol. 21, no. 4, pp. 195–206, Apr. 1981, doi: 10.1016/0011-2275(81)90195-8.
[2] L. J. M. van de Klundert and H. H. J. ten Kate, “On fully superconducting rectifiers and fluxpumps. A review. Part 2: Commutation modes, characteristics and switches,” Cryogenics, vol. 21, no. 5, pp. 267–277, May 1981, doi: 10.1016/0011-2275(81)90002-3.
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[4] J. Geng, C. W. Bumby, and R. A. Badcock, “Maximising the current output from a self-switching kA-class rectifier flux pump,” Supercond. Sci. Technol., vol. 33, no. 4, p. 045005, Apr. 2020, doi: 10.1088/1361-6668/ab6957.
[5] G. B. J. Mulder, H. H. J. ten Kate, H. J. G. Krooshoop, and L. J. M. van de Klundert, “Development of a thermally switched superconducting rectifier for 100 kA,” IEEE Trans. Magn., vol. 27, no. 2, pp. 2333–2336, Mar. 1991, doi: 10.1109/20.133685.
[6] A. J. Creely et al., “Overview of the SPARC tokamak,” J. Plasma Phys., vol. 86, no. 5, p. 865860502, Oct. 2020, doi: 10.1017/S0022377820001257.

Acknowledgment

This work was supported in part by the New Zealand Ministry of Business, Innovation and Employment (MBIE RTVU1916), and has been part-funded by STEP, a UKAEA programme to design and build a prototype fusion energy plant and a path to commercial fusion.