In embodiments of the invention, a superconductor lead is configured to have less ohmic heating by its own current and less heat conduction from room temperature to cryogenic temperature, where a cryogenic apparatus is located. The superconducting lead with no ohmic resistance and low thermal conduc
In embodiments of the invention, a superconductor lead is configured to have less ohmic heating by its own current and less heat conduction from room temperature to cryogenic temperature, where a cryogenic apparatus is located. The superconducting lead with no ohmic resistance and low thermal conductivity disclosed herein maximizes current capacity by placing superconductors in parallel, each having equal current. Thus, the resistances are controlled to provide uniform current distribution through each superconductor of the high temperature superconducting (HTS) lead.
대표청구항▼
1. A high temperature superconducting (HTS) lead for use in transmitting current from room temperature to cryogenic temperatures, comprising: two or more superconductors positioned in parallel, each superconductor having a first end and a second end;at least two electrical connectors, one connected
1. A high temperature superconducting (HTS) lead for use in transmitting current from room temperature to cryogenic temperatures, comprising: two or more superconductors positioned in parallel, each superconductor having a first end and a second end;at least two electrical connectors, one connected at said first end and one connected at said second end;wherein each said superconductor has a current distribution controlled by resistance between the electrical connector and each of said first end and said second end of the superconductor, each said superconductor transmitting equivalent current. 2. The HTS lead of claim 1, wherein a combination of the current distribution through the superconductors has a total lead current capacity that is maximized by the equivalent current distributed through each superconductor. 3. The HTS lead of claim 1, wherein said first end is a warm end and said second end is a cold end. 4. The HTS lead of claim 1, wherein at least one electrical conductor of the two electrical connectors is a copper terminal. 5. The HTS lead of claim 4, wherein the copper terminal takes the shape of a fork with a slit between at least two prongs. 6. The HTS lead of claim 5, wherein the fork is multi-pronged. 7. The HTS lead of claim 4, wherein the copper terminal is compressed to the two or more superconductors at said first end or said second end with a resistive element sandwiched therebetween. 8. The HTS lead of claim 7, wherein the resistive element is Indium. 9. The HTS lead of claim 7, wherein the copper terminal is soldered to the two or more superconductors with a resistive element sandwiched therebetween. 10. The HTS lead of claim 9, wherein the resistive element is stainless steel, brass, other alloy materials, or combinations thereof. 11. The HTS lead of claim 1, wherein the at least two electrical conductors comprise one or more of a multi-prong copper conductor, at least one electrical conductor compressed to the two or more superconductors at said warm end or said cold end with a resistive element sandwiched therebetween, and at least one electrical conductor soldered to the two or more superconductors at said warm end or said cold end with a resistive element sandwiched therebetween, alone or in combination. 12. A method of distributing current uniformly through two or more superconductors comprising the steps of: providing the HTS lead of claim 1; andtransmitting current from a power supply at room temperature through said superconductors to a cryogenic apparatus at cryogenic temperature, such that current distribution is uniform throughout the HTS lead. 13. The method of claim 12, further comprising a step of controlling resistance at the electrical connectors to provide equivalent current through each superconductor. 14. A method of measuring current in each of the two or more superconductors of the high temperature superconducting (HTS) lead in claim 1, the method comprising the steps of: providing a magnetic measurement probe at the superconductors to scan a magnetic field; andacquiring magnetic field measurements generated by the current in each of the superconductors before the current reaches respective critical currents of each of the superconductors. 15. The method of claim 14, wherein the magnetic measurement probe is a Hall probe that moves in a direction to scan the magnetic field. 16. The method of claim 14, wherein the magnetic measurement probe slides over the superconductors and measures current distribution by sensing the magnetic field generated by the current in each of the superconductors. 17. The method of claim 14, further comprising a step of acquiring a field distribution where uneven current sharing is present. 18. The method of claim 17, further comprising a step of adjusting resistance at the electrical connectors using the magnetic field measurements. 19. The method of claim 18, wherein the step of adjusting resistance, the field distribution provides even current sharing between each superconductor.
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