Radio frequency-assisted fast superconducting switch

• US 9,837,814 B2
• Filed: 04/09/2013
• Issued: 12/05/2017
• Est. Priority Date: 04/11/2012
• Status: Expired due to Fees

• Current Assignee: Brookhaven Science Associates, LLC (Government of the United States of America)
• Original Assignee: Brookhaven Science Associates, LLC (Government of the United States of America)
• Inventors: Solovyov, Vyacheslav, Li, Qiang
• Primary Examiner(s): Jackson, Stephen W
• Assistant Examiner(s): CLARK, CHRISTOPHER JAY
• Application Number:
  US14/385,094
• Publication Number:
  US 20150045228A1
• Time in Patent Office: 1,701 Days
• CPC Class Codes: H02H 9/023 Current limitation using superconducting elements
• CPC Class Codes: H03K 17/92 by the use, as active elements, of superconductive devices
• CPC Class Codes: H10N 60/355 Power cryotrons
• CPC Class Codes: Y10T 29/49014 Superconductor

Abstract

A radio frequency-assisted fast superconducting switch is described. A superconductor is closely coupled to a radio frequency (RF) coil. To turn the switch “off,” i.e., to induce a transition to the normal, resistive state in the superconductor, a voltage burst is applied to the RF coil. This voltage burst is sufficient to induce a current in the coupled superconductor. The combination of the induced current with any other direct current flowing through the superconductor is sufficient to exceed the critical current of the superconductor at the operating temperature, inducing a transition to the normal, resistive state. A by-pass MOSFET may be configured in parallel with the superconductor to act as a current shunt, allowing the voltage across the superconductor to drop below a certain value, at which time the superconductor undergoes a transition to the superconducting state and the switch is reset.

Claims

1. A superconducting switch, comprising:

a superconducting tape;

a radio frequency (RF) coil strongly coupled to the superconducting tape, where the superconducting tape is tightly wrapped around the RF coil with at least one undulation forming at least one smooth turn around the RF coil; and

an RF inverter that induces a voltage burst in the RF coil, where the voltage burst induces a RF-induced current in the superconducting tape, where the RF-induced current and a direct current in the superconducting tape exceed a critical current of the superconductor tape at an operating temperature.

2. The superconducting switch of claim 1, wherein the superconducting switch is a superconducting fault current limiter.

3. The superconducting switch of claim 1, wherein the superconducting tape is superconductive at temperatures above 60 K.

4. The superconducting switch of claim 1, wherein the superconducting tape is made from yttrium barium copper oxide (YBCO;

Tc=93 K) or bismuth strontium calcium copper oxide (BiSCCO;

Bi-2212 has Tc≈

95 K, Bi-2223 has Tc≈

108 K, and Bi-2234 has Tc≈

104K) to form a superconducting layer deposited on a substrate made from nickel, nickel-tungsten alloy, stainless steel, or superalloy.

5. The superconducting switch of claim 1, wherein the RF coil is made from a material that can carry alternating current at frequencies up to about 1 MHz.

6. The superconducting switch of claim 5, wherein the RF coil is made from a race-track shaped RF coil wound from multi-strand Litz wire.

7. The superconducting switch of claim 1, further comprising:

a by-pass MOSFET coupled in parallel with the superconducting tape, wherein the by-pass MOSFET is operable to provide a low-resistance shunt to the superconducting tape that prevents damage of a superconducting layer during transition of the superconducting tape into the normal state from the superconducting state and into the superconducting state from the normal state.

8. The superconducting switch of claim 1, wherein a switching time of the superconducting tape from a superconducting into a normal state is less than 5 ms.

9. The superconducting switch of claim 8, wherein the switching time of the superconducting tape from its normal state into its superconducting state is less than 5 ms.

10. The superconducting switch of claim 1, having an ″

off resistance of greater than 10 kΩ

.

11. A method of fabricating a fast superconducting switch, the method comprising:

strongly coupling a radio frequency (RF) coil to a superconducting tape by tightly wrapping the superconducting tape around the RF coil with at least one undulation forming at least one smooth turn around the RF coil;

connecting the RF coil to an RF inverter, such that

the RF inverter is operable to induce a voltage burst in the RF coil, where the voltage burst induces a RF-induced current in the superconducting tape, where the RF-induced current and the direct current in the superconducting tape exceed a critical current of the superconducting tape at an operating temperature.

12. A method of operating a superconducting switch, the method comprising:

applying a high-frequency voltage burst to a radio frequency (RF) coil,

wherein the RF coil is strongly coupled to a superconducting tape by tightly wrapping the superconducting tape around the RF coil with at least one undulation forming at least one smooth turn around the RF coil,

the superconducting tape has flowing through it a direct current with a magnitude less than a critical current of the superconducting tape at an operating temperature,

the high-frequency voltage burst is sufficient to induce a RF-induced current in the superconducting tape, the sum of the RF-induced current and the direct current exceeding the critical current of the superconducting tape at the operating temperature, and

whereby the superconducting tape excited with the RF-induced current undergoes a transition from a superconducting state to a normal state.

13. The method of claim 12 further comprising:

configuring a by-pass MOSFET in parallel with the superconducting tape, such that the bypass MOSFET is operable to shunt current from the superconducting tape that prevents damage of a superconducting layer during transition of the superconducting tape into its normal state, and reduces the voltage across the superconducting tape below a certain value which allows the superconducting switch to become superconducting.

14. The method of claim 13, wherein the transition from the superconducting state into the normal state of the superconducting tape takes less than 5 ms.

15. The method of claim 14, wherein when the direct current and the RF-induced current are shunted from the superconducting tape the critical current of the superconducting tape is no longer exceeded and the superconducting tape undergoes a transition into its superconducting state from its normal state.

16. The method of claim 15, wherein the transition into the superconducting state of the superconducting tape takes less than 5 ms.