IP Library › Granted Patent US 12,568,774
Granted Patent B2
US 12,568,774 · App. 18/272,972 · Granted Mar 3, 2026

Superconducting switches

Inventors: Rodney Alan Badcock (Wellington, NZ); Christopher William Bumby (Wellington, NZ); Jianzhao Geng (Hubei, CN); James Hamilton Palmer Rice (Wellington, NZ)
Assignee: VICTORIA LINK LIMITED
H10N60/84H10N60/35H10N60/83
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Quick Facts
Patent No.
US 12,568,774
App. No.
18/272,972
Granted
Mar 3, 2026
Kind
B2
Abstract

There is provided an electrical switch comprising a length of superconducting material. In some forms the electrical switch is configured to be controlled between a low-resistance state and a higher-resistance state by the selective application of one or more switching mechanisms. In the higher-resistance state, current flowing through the length of superconducting material may approach the critical current of the length of superconducting material, may be substantially equal to the critical current or may be greater than the critical current. In some forms, the length of superconducting material is a length of high temperature superconducting material. The switching mechanisms may comprise: heating the length of superconducting material; applying a magnetic field to the length of superconducting material; applying a time-varying magnetic field to create dynamic resistance and/or heat; and/or applying a time-varying magnetic field to a loop of superconducting material to create a screening current around the loop.

Claims (49)

1 . An electrical switch comprising:

a length of superconducting material configured to carry a transport current, wherein the length of superconducting material has a critical current and a critical temperature;

a magnetic field generator configured to apply a magnetic field to the length of superconducting material; and

a heating assembly for heating the length of superconducting material,

wherein the magnetic field generator and the heating assembly are configured to be selectively controlled independently or in combination to switch the length of superconducting material between a low-resistance state and a higher resistance state,

wherein, in the low-resistance state, a magnitude of the magnetic field is relatively low and a temperature of the length of superconducting material is substantially less than the critical temperature such that the transport current is substantially less than the critical current,

wherein, in a first configuration of the electrical switch in the higher-resistance state, the magnitude of the magnetic field is relatively high to reduce the critical current;

wherein, in a second configuration of the electrical switch in the higher-resistance state, the heating assembly heats the length of superconducting material to reduce the critical current,

wherein, in a third configuration of the electrical switch in the higher-resistance state, the magnitude of the magnetic field is relatively high and the heating assembly heats the length of superconducting material to reduce the critical current, and

wherein, in each of the configurations of the electrical switch in the higher-resistance state, the critical current is reduced such that the transport current approaches the critical current, is substantially equal to the critical current or is greater than the critical current of the length of superconducting material.

2 . An electrical switch as claimed in claim 1 , wherein the magnetic field generator and the heating assembly are configured to be selectively activated and de-activated independently or in combination to switch the electrical switch between the low-resistance state and the higher resistance state.

3 . An electrical switch as claimed in claim 2 , wherein the heating assembly is configured to remain activated and the length of superconducting material is switched between the low-resistance state and the higher-resistance state by selective de-activation and activation of the magnetic field generator.

4 . An electrical switch as claimed in claim 1 , wherein the magnetic field applied by the magnetic field generator is a constant magnetic field.

5 . An electrical switch as claimed in claim 1 , wherein the heating assembly comprises a resistive heating element positioned in thermal contact with the length of superconducting material.

6 . An electrical switch as claimed in claim 1 , wherein the superconducting material is a high-temperature superconducting material.

7 . An electrical switch as claimed in claim 1 , wherein the magnetic field generator is a first magnetic field generator and the magnetic field is a first magnetic field, and wherein the electrical switch comprises a second magnetic field generator configured to apply a second, time-varying, magnetic field to the length of superconducting material, wherein the second magnetic field generator is configured to be selectively controlled to switch the length of superconducting material between the low-resistance state and the higher resistance state.

8 . An electrical switch as claimed in claim 7 , wherein the superconducting material is a tape having two opposed faces, and wherein the second magnetic field generator is configured to apply the second magnetic field in a direction substantially perpendicular to the two opposed faces.

9 . An electrical switch as claimed in claim 7 , wherein the first magnetic field generator and the second magnetic field generator are the same magnetic field generator, wherein the magnitude of the magnetic field applied by the same magnetic field generator varies in time with a DC bias.

10 . An electrical switch as claimed in claim 1 , wherein:

the length of superconducting material comprises a loop of superconducting material configured to carry the transport current between a first terminal and a second terminal, wherein the loop comprises a first branch and a second branch, the first and second branches being electrically connected in parallel between the first terminal and the second terminal, and wherein the loop has an axis which is substantially normal to the plane of the loop, and

the electrical switch further comprises:

a third, time-varying, magnetic field generator configured to apply a third, time-varying, magnetic field through the loop with the direction of the third magnetic field through the loop being generally parallel to, or having a component which is generally parallel to, the axis of the loop,

wherein, in the low-resistance state, the third magnetic field generator does not apply the third magnetic field through the loop and the transport current flows through the loop between the two terminals, and

wherein, in the higher-resistance state, the third magnetic field generator applies the third magnetic field through the loop, inducing a screening current in the loop such that a total current in one or more of the first branch and the second branch approaches the critical current, is substantially equal to the critical current or is greater than the critical current of the superconducting material.

11 . An electrical switch as claimed in claim 1 , wherein, in the higher-resistance state, the length of superconducting material is in a superconducting state.

12 . An electrical switch comprising:

a length of superconducting material configured to carry a transport current, wherein the length of superconducting material has a critical current and a critical temperature;

a first magnetic field generator configured to apply a first, constant, magnetic field to the length of superconducting material; and

a second magnetic field generator configured to apply a second, time-varying, magnetic field to the length of superconducting material,

wherein the first magnetic field generator and the second magnetic field generator are configured to be selectively controlled independently or in combination to switch the length of superconducting material between a low-resistance state and a higher resistance state,

wherein, in the low-resistance state, magnitudes of the first magnetic field and the second magnetic field are relatively low and the transport current is substantially less than the critical current,

wherein, in a first configuration of the electrical switch in the higher-resistance state, the magnitude of the first magnetic field is relatively high to reduce the critical current such that the transport current approaches the critical current, is substantially equal to the critical current or is greater than the critical current of the length of superconducting material,

wherein, in a second configuration of the electrical switch in the higher-resistance state, the second magnetic field creates dynamic resistance in the length of superconducting material, and

wherein, in a third configuration of the electrical switch in the higher-resistance state, the magnitude of the first magnetic field is relatively high to reduce the critical current such that the transport current approaches the critical current, is substantially equal to the critical current or is greater than the critical current of the length of superconducting material, and the second magnetic field creates dynamic resistance in the length of superconducting material.

13 . An electrical switch as claimed in claim 12 , wherein the first magnetic field generator and the second magnetic field generator are configured to be selectively activated and de-activated independently or in combination to switch the length of superconducting material between the low-resistance state and the higher resistance state.

14 . An electrical switch as claimed in claim 13 , wherein the first magnetic field generator is configured to remain activated and the length of superconducting material is switched between the low-resistance state and the higher-resistance state by selective de-activation and activation of the second magnetic field generator.

15 . An electrical switch as claimed in claim 13 , wherein the second magnetic field generator is configured to remain activated and the length of superconducting material is switched between the low-resistance state and the higher-resistance state by selective de-activation and activation of the first magnetic field generator.

16 . An electrical switch as claimed in claim 12 , wherein the superconducting material is a tape having two opposed faces, and wherein the second magnetic field generator is configured to apply the second magnetic field in a direction substantially perpendicular to the two opposed faces.

17 . An electrical switch as claimed in claim 12 , wherein the first magnetic field generator and the second magnetic field generator are the same magnetic field generator, wherein the magnitude of the magnetic field applied by the same magnetic field generator varies in time with a DC bias.

18 . An electrical switch as claimed in claim 12 , wherein the superconducting material is a high-temperature superconducting material.

19 . An electrical switch as claimed in claim 12 , wherein the electrical switch further comprises a heating assembly for heating the length of superconducting material, wherein, in the higher-resistance state, the heating assembly heats the length of superconducting material to reduce the critical current such that the transport current approaches the critical current, is substantially equal to the critical current or is greater than the critical current of the length of superconducting material.

20 . An electrical switch as claimed in claim 19 , wherein the heating assembly comprises a resistive heating element positioned in thermal contact with the length of superconducting material.

21 . An electrical switch as claimed in claim 12 , wherein:

the length of superconducting material comprises a loop of superconducting material configured to carry the transport current between a first terminal and a second terminal, wherein the loop comprises a first branch and a second branch, the first and second branches being electrically connected in parallel between the first terminal and the second terminal, and wherein the loop has an axis which is substantially normal to the plane of the loop, and

the electrical switch further comprises:

a third, time-varying, magnetic field generator configured to apply a third, time-varying, magnetic field through the loop with the direction of the third magnetic field through the loop being generally parallel to, or having a component which is generally parallel to, the axis of the loop,

wherein, in the low-resistance state, the third magnetic field generator does not apply the third magnetic field through the loop and the transport current flows through the loop between the two terminals, and

wherein, in the higher-resistance state, the third magnetic field generator applies the third magnetic field through the loop, inducing a screening current in the loop such that a total current in one or more of the first branch and the second branch approaches the critical current, is substantially equal to the critical current or is greater than the critical current of the superconducting material.

22 . An electrical switch as claimed in claim 12 , wherein, in the higher-resistance state, the length of superconducting material is in a superconducting state.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 18, 2023
From: BADCOCK, RODNEY ALAN; BUMBY, CHRISTOPHER WILLIAM; GENG, JIANZHAO; RICE, JAMES HAMILTON PALMER
To: VICTORIA LINK LIMITED
Reel/Frame 065262/0472 →
Priority Claims (3)
AU 2021900162 · Jan 26, 2021 · national
AU 2021900163 · Jan 26, 2021 · national
AU 2021903413 · Oct 26, 2021 · national
Continuity (1)
Related Publication 20240090349A1 · Mar 14, 2024
References Cited (35)
US 3384762A · Mawardi · 1968 [cited by applicant]
US 4122512A · Peterson et al. · 1978 [cited by applicant]
US 4348630A · Boenig et al. · 1982 [cited by applicant]
US 5036042A · Hed · 1991 [cited by applicant]
US 5107240A · Tashiro et al. · 1992 [cited by applicant]
US 5241447A · Barber · 1993 [cited by examiner]
US 5805036A · Hodge et al. · 1998 [cited by applicant]
US 6147579A · Einziger et al. · 2000 [cited by applicant]
US 8384504B2 · Diederichs et al. · 2013 [cited by applicant]
US 10269478B2 · Geng · 2019 [cited by examiner]
US 12439833B2 · Badcock · 2025 [cited by examiner]
US 20020017970A1 · Kinder · 2002 [cited by applicant]
US 20070127171A1 · Lee · 2007 [cited by examiner]
US 20080204671A1 · Jeitner · 2008 [cited by applicant]
US 20120010083A1 · Vaucher · 2012 [cited by applicant]
US 20130096008A1 · Bright et al. · 2013 [cited by applicant]
US 20160197471A1 · Klaus · 2016 [cited by examiner]
US 20170069415A1 · Faley et al. · 2017 [cited by applicant]
US 20180218818A1 · Geng et al. · 2018 [cited by applicant]
IN 320055 · 2011 [cited by applicant]
JP 2003069093A · 2003 [cited by applicant]
WO 1997026668 · 1997 [cited by applicant]
WO 03056381A1 · 2003 [cited by applicant]
WO 2021080443 · 2021 [cited by applicant]
Partial Supplementary European Search Report in EP Application No. 22746334.6-1211/4272267, mailed Dec. 19, 2024 (13 pages). [cited by applicant]
Extended European Search Report in EP Application No. 22746334.6-1211/4272267, mailed Apr. 4, 2025 (12 pages). [cited by applicant]
Jianzhao Geng, “A wireless rectifier for inductively energizing high direct-current high-temperature superconducting magnets”, IEEE Transactions on Industrial Electronics, vol. 68, No. 4, Mar. 25, 2020, 3273-3281. [cited by applicant]
International Search Report and Written Opinion in corresponding International Patent Application No. PCT/NZ2021/050008, mailed Apr. 19, 2022 (11 pages). [cited by applicant]
Chao Li et al: “Design for a Persistent Current Switch Controlled by Alternating Current Magnetic Field”, IEEE Transactions on Applied Superconductivity, vol. 28, No. 4, Jun. 2018, p. 1-5. Whole document, especially abs… [cited by applicant]
Maximising the current output from a self-switching kA-class rectifier flux pump, Jianzhao Geng et al, 2020 Supercond Sci Technol 33-045005. [cited by applicant]
An HTS flux pump by directly driving a superconductor into a flux flow region in the E-J curve, Jianzhao Geng and T A Coombs, May 6, 2016 Supercond Sci Technol 29-095004. [cited by applicant]
Dynamic resistance of YBCO-coated conductors in applied AC fields with DC transport currents and DC background fields, Duckworth et al, IEEE Transactions on Applied Superconductivity, vol. 21, No. 3, Jun. 2011. [cited by applicant]
Active Quenching Technique for YBCO Tapes: Quench Acceleration and Protection, X. Zhang et al, Journal of Superconductivity and Novel Magnetism (2018) 31:3465-3474, Mar. 19, 2018, pp. 3465-3474. [cited by applicant]
A Flux Pump for NMR Magnets, Haigun Lee et al., IEEE Transactions on Applied Superconductivity, 13, Jun. 2003. [cited by applicant]
A Circuit Analysis of a Flux Pump, Archie Campbell, Superconductor Science and Technology, 32, Oct. 7, 2019. [cited by applicant]