Claims
- 1. A device including:
- a type II superconductor,
- a magnet,
- a conductor through which an electrical current can flow to produce a magnetic field intercepting said superconductor to alter the flux penetration properties of said superconductor, said magnet being capable of suspension or levitation with respect to said superconductor, the levitation or suspension distance being continuously adjustable over a range depending on the magnitude of electrical current through said conductor.
- 2. The device of claim 1, where said superconductor is a high T.sub.c superconductor.
- 3. The device of claim 2, where said superconductor contains copper-oxygen current-carrying planes.
- 4. The device of claim I, where said superconductor is a metal or metal alloy.
- 5. The device of claim 1, where said conductor is a coil surrounding said superconductor.
- 6. The device of claim 1, where the magnetic field produced by the current in said conductor intercepts a substantial portion of said superconductor.
- 7. The device of claim 1, where said conductor and said magnet are located on opposite sides of said superconductor.
- 8. The device of claim 1, where said conductor is substantially coplanar with a surface of said superconductor.
- 9. The device of claim 1, where the magnetic field produced by said conductor includes a component substantially perpendicular to a surface of said superconductor.
- 10. A high T.sub.c superconductor-magnet system for suspension or levitation, comprising: a high t.sub.c superconductor, a magnet, an electrical conductor for carrying an electrical current therein which produces a magnetic field H intercepting at least a portion of said superconductor and affecting the flux penetration properties of said superconductor, and a current means for producing said electrical current in said conductor, said current means being capable of producing an electrical current of varying magnitude for altering the levitation or suspension distance between said magnet and said superconductor and wherein, said magnetic field H is in the range H.sub.c1 <H<H.sub.c2 where H.sub.c1 and H.sub.c2 are the lower and upper critical fields of said superconductor.
- 11. The system of claim 10, where said electrical conductor and said magnet are located on opposite sides of said superconductor.
- 12. A high T.sub.c superconductor-magnet system for suspension or levitation, comprising: a high t.sub.c superconductor, a magnet, an electrical conductor for carrying an electrical current therein which produces a magnetic field intercepting at least a portion of said superconductor and affecting the flux penetration properties of said superconductor, and a current means for producing said electrical current in said conductor, said current means being capable of producing an electrical current of varying magnitude for altering the levitation or suspension distance between said magnet and said superconductor and wherein, said electrical conductor surrounds said superconductor.
- 13. The system of claim 10, further including cooling means for cooling said superconductor.
- 14. The system of claim 10, where said conductor forms a coil, the axis of said coil being substantially perpendicular to a surface of said superconductor.
- 15. The system of claim 10, where said conductor forms a coil, the axis of said coil being at an angle between 0.degree. and 90.degree. with respect to a surface of said superconductor.
- 16. An apparatus including in combination:
- a member having a magnetic moment associated herewith,
- a high T.sub.c superconductor,
- electrical means for controllably producing a magnetic field intercepting said superconductor and of sufficient magnitude to alter the flux penetration properties of said superconductor,
- said electrical means being controllable to produce a magnetic field H of varying strength to vary the levitation or suspension effects between said member and said superconductor and wherein said magnetic field H produced by said electrical means is in the range H.sub.c1 <H<H.sub.c2 where H.sub.c1 and H.sub.c2 are the lower and upper critical fields of said superconductor.
- 17. A device including:
- a type II superconductor,
- a magnet said magnet and said superconductor forming a magnet-superconducting system,
- a conductor through which an electrical current can flow to produce a magnetic field entering said magnet-superconductor system, said magnet being capable of suspension or levitation with respect to said superconductor, the levitation or suspension distance being continuously adjustable over a range depending on the magnitude of electrical current through said conductor.
- 18. The device of claim 17, where said superconductor is a high T.sub.c superconductor.
- 19. The device of claim 17, where said magnet is levitated, said magnet being levitated at a position between said superconductor and said conductor.
- 20. The device of claim 17, where said conductor is a coil.
- 21. A high T.sub.c superconductor-magnet system for suspension or levitation comprising: a high T.sub.c superconductor, a magnet, said high T.sub.c superconductor and said magnet forming a high T.sub.c superconductor-magnetic system, an electrical conductor for carrying an electrical current therein which produces a magnetic field H intercepting said magnet for affecting interactions in said high T.sub.c superconductor-magnet system, and a current means for producing said electrical current in said conductor, said current means being capable of producing an electrical current of varying magnitude for altering the levitation or suspension distance between said magnet and said superconductor, wherein said magnetic field H is in the range H.sub.c1 H<H.sub.c2 where H.sub.c1 and H.sub.c2 are the lower and upper critical fields of said superconductor.
- 22. The system of claim 21, where said electrical conductor is located on the same side of said high T.sub.c superconductor as said magnet.
- 23. The system of claim 21, where said electrical conductor is a coil.
- 24. The system of claim 23, where the axis of said coil is substantially perpendicular to a surface of said superconductor.
- 25. The system of claim 23, where the axis of said coil is at an angle between 0 degrees and 90 degrees with respect to a surface of said superconductor.
- 26. An apparatus including in combination:
- a member having a magnetic moment associated herewith,
- a high T.sub.c superconductor,
- electrical means for controllably producing a magnetic field intercepting said superconductor and of sufficient magnitude to alter the flux penetration properties of said superconductor,
- said electrical means being controllable to produce a magnetic field of varying strength to vary the rotational displacement of said member with respect to said superconductor.
- 27. The apparatus of claim 26, where said member is levitated, said electrical means being a coil.
- 28. The apparatus of claim 27, where said member is levitated to a position between said coil and said superconductor.
- 29. A device including:
- a type II supeconductor,
- a magnet,
- a conductor through which an electrical current can flow to produce a magnetic field intercepting said superconductor to alter the flux penetration properties of said superconductor, said magnet being capable of suspension or levitation with respect to said superconductor, the levitation or suspension distance being continuously adjustable over a range depending on the magnitude of electrical current through said conductor, and
- a magnetic element to modify the magnetic field at said superconductor,
- said magnetic element includes a plate of magnetic material.
- 30. The device of claim 29 further including means for moving said plate of magnetic material with respect to said superconductor whereby said magnet is moved with respect to said superconductor.
- 31. A device including:
- a type II superconductor,
- a magnet,
- a magnetic element, and
- means for positioning said magnetic element with respect to said superconductor to alter the flux penetration properties of said superconductor, said magnet being capable of suspension or levitation with respect to said superconductor, the levitation or suspension distance being continuously adjustable over a range depending on the position of said magnetic element, said magnetic element includes a plate of magnetic material.
- 32. The device of claim 31, where said superconductor is a high T.sub.c superconductor.
- 33. The device of claim 32, where said superconductor contains copper-oxygen current-carrying planes.
- 34. The device of claim 31, where said superconductor is a metal or metal alloy.
- 35. The device of claim 31 further including a conductor through which an electrical current can flow to produce a magnetic field intercepting said superconductor to alter the flux penetration properties of said superconductor.
- 36. The device of claim 35, where said conductor is a coil surrounding said superconductor.
- 37. The device of claim 35, where the magnetic field produced by said conductor includes a component substantially perpendicular to a surface of said superconductor.
- 38. The device of claim 31 including means for moving said magnetic element with respect to said superconductor from a first position to a second position whereby said magnet is moved with respect to said superconductor.
Parent Case Info
This application is a CIP of Ser. No. 07/919,702, filed Jul. 24, 1992, now abandoned, which is a CIP of Ser. No. 07/370,487, filed Jun. 23, 1989, now abandoned.
Government Interests
This application is a CIP of Ser. No. 07/919,702, filed Jul. 24, 1992, now abandoned, which is a CIP of Ser. No. 07/370,487, filed Jun. 23, 1989, now abandoned.
US Referenced Citations (7)
Foreign Referenced Citations (2)
Number |
Date |
Country |
404147 |
Dec 1990 |
EPX |
299760 |
Dec 1988 |
JPX |
Continuations (1)
|
Number |
Date |
Country |
Parent |
451915 |
Dec 1989 |
|
Continuation in Parts (2)
|
Number |
Date |
Country |
Parent |
919702 |
Jul 1992 |
|
Parent |
370487 |
Jun 1989 |
|