US3253192A - Superconducting solenoid apparatus - Google Patents
Superconducting solenoid apparatus Download PDFInfo
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- US3253192A US3253192A US309986A US30998663A US3253192A US 3253192 A US3253192 A US 3253192A US 309986 A US309986 A US 309986A US 30998663 A US30998663 A US 30998663A US 3253192 A US3253192 A US 3253192A
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- core
- gap
- superconducting
- coil
- temperature
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- 239000000463 material Substances 0.000 claims description 13
- 230000005294 ferromagnetic effect Effects 0.000 claims description 12
- 239000012530 fluid Substances 0.000 claims description 5
- 230000005291 magnetic effect Effects 0.000 claims description 4
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 7
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 4
- 229910052802 copper Inorganic materials 0.000 description 4
- 239000010949 copper Substances 0.000 description 4
- 229910052734 helium Inorganic materials 0.000 description 4
- 239000001307 helium Substances 0.000 description 4
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 4
- 238000010438 heat treatment Methods 0.000 description 2
- 229910052742 iron Inorganic materials 0.000 description 2
- 239000007788 liquid Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 239000002887 superconductor Substances 0.000 description 2
- 238000004804 winding Methods 0.000 description 2
- 229910020018 Nb Zr Inorganic materials 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 230000008020 evaporation Effects 0.000 description 1
- 238000001704 evaporation Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 229910052758 niobium Inorganic materials 0.000 description 1
- 239000010955 niobium Substances 0.000 description 1
- GUCVJGMIXFAOAE-UHFFFAOYSA-N niobium atom Chemical compound [Nb] GUCVJGMIXFAOAE-UHFFFAOYSA-N 0.000 description 1
- 230000005298 paramagnetic effect Effects 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
- 238000005245 sintering Methods 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
- H01F6/02—Quenching; Protection arrangements during quenching
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10S505/00—Superconductor technology: apparatus, material, process
- Y10S505/825—Apparatus per se, device per se, or process of making or operating same
- Y10S505/85—Protective circuit
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10S505/00—Superconductor technology: apparatus, material, process
- Y10S505/825—Apparatus per se, device per se, or process of making or operating same
- Y10S505/879—Magnet or electromagnet
Definitions
- Such coils are subject to electrical energy losses in lead wires connected to the superconductive material, the soldered connections of such lead wires and the power supply and evaporation losses due to resistance heating in proximity to the cryogenic fluid.
- the drawing consists of a single figure which is a schematic diagram of ⁇ a magnet constructed according to a preferred embodiment of the invention.
- the magnet comprises a soft iron core 10, including a movable pole piece 12 which may be moved into the position shown in dotted lines to form a closed magnetic loop.
- Currents are induced in the core by a copper coil 14 connected to a suitable power supply 16.
- the superconducting solenoid 18 comprises closed loops, which may be cylinders as shown in the drawing or closed loop wires.
- the cylinders can be made of formed and sintered NjbBSn powders or extruded Nb-Zr tubing. Non-superconductor cylinders should be provided to radially separate the superconductive cylinders. Copper is a preferred choice for this purpose. Where wire is used, it can be of the type described by Kunzler et al. in 6 Physical Review 89 (1961). However, the wires should be formed into closed loops before sintering.
- the superconducting coil is held in a Dewar flask 20 of annular form which is placed around a pole piece of the core 10.
- this magnet assembly begins with the pole piece 12 closing the air gap of the magnet and the temperature ofthe superconductive coil above the critical temperature of Iits constituent material. Power is supplied to the copper coil to induce a eld in the iron core up to its saturation limit. Then helium is supplied to the Dewar 20 to lower the temperature of the coil 18 below the critical temperature. So far, no current flows in the superconducting coil.
- the copper coil is then cut off from the power supply. This causes -a small current to be induced in the superconducting coil, but the iron core remains saturated. Then the air gap is opened by lowering the pole piece 12. Additional current is induced in the .superconducting coil and the constant flow of current without resistance maintains the high field across the air gap. The field in the gap is maintained so long as the coil is kept at liquid helium temperature and the ⁇ air gap spacing is not too great. When the air gap spacing is excessive, the coil 18 will go normal. The current in the coils will cause a resistive heating which is dissipated by helium boil-off. The superconductive loops will not burn out.
- the pole piece 12 can be rigidly attached to the remainder of core 10 and the air gap lled by a removable iron keeper.
- the superconductive loops can be simple niobium cylinders or hard superconductor alloys made by the diffusion technique described by Saur in Die Naturwissenschaften, 49, p. 129 (1962).
- the location of the superconducting coil near a pole face, as shown in the drawing, is preferred to reduce stray flux when the air gap is opened. However, this location is not critical to the invention.
- a superconducting magnet characterized by burnout proof protection for superconductive windings and freedom from relatively low critical current capacity section, such as joints, and comprising, in combination: a ferromagnetic core with a magnet gap, means for creating a magnetic field in the core, a superconducting coil electromagnetically linked to the ferromagnetic core, the coil comprising closed rings of superconducting material in an essentially closed space, a cryogenic fluid having a temperature below the critical temperature of the superconducting material, means for admitting said cryogenic iiuid to said space for lowering the temperature of the coil below the critic-al temperature of the superconducting material, a portion of said ferromagnetic core being movable relative to the rest of the core between at least a first position wherein the core has said magnet gap and a second position wherein said gap is closed, with said core portion providing a consistently large cross-section area for bridging the gap in said second position, and means connected to said core portion and constructed and arranged to move said core portion
- a superconducting magnet characterized by burnout proof protection for superconductive windings and freedom from relatively low critical current capacity section, such as joints, and comprising in combination: a closed loop ferromagnetic core, a superconducting coil electromagnetically linked to the ferromagnetic core, the coil comprising closed rings of superconducting material in an essentially closed space, a cryogenic uid having a temperature below the critical temperature of the superconducting material, means for admitting said cryogenic uid to said space for lowering the temperature of the coil below the critical temperature of the superconducting material, means forming a portion of said closed loop ferromagnetic core of consistently large cross-section area, said means being constructed and arranged so that it is removable from the core to leave a magnet gap in the core when it is removed.
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- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Containers, Films, And Cooling For Superconductive Devices (AREA)
Description
May 24, 1966 L RINDERER 3,253,192
SUPERGONDUCTING SOLENOID APPARATUS Filed sept. 19, 1963 United States Patent O 3,253,192 SUPERCONDUCTING SOLENOD APPARATUS Leo Rinderer, Lausanne, Switzerland, assigner to National Research Corporation, Cambridge, Mass., a corporation of Massachusetts Filed Sept. 19, 1963, Ser. No. 309,986 2 Claims. (Cl. S17- 158) The present invention relates to superconducting magnets and specifically to a technique of building up a magnetic field and maintaining it with superconductive coils.
In the present state of the `art superconductive materials are wound into coils about ferromagnetic or paramagnetic cores. A current is passed through the coil from a power supply and then short circuited. Meanwhile the superconductive material is maintained below its critical temperature by a cryogenic fluid, such as liquid helium.
Such coils are subject to electrical energy losses in lead wires connected to the superconductive material, the soldered connections of such lead wires and the power supply and evaporation losses due to resistance heating in proximity to the cryogenic fluid.
It is an object of the p-resent invention to provide a magnet construction which inherently avoids these losses.
It is another object of the invention to provide a superconductive solenoid which will not burn out due to an accidental instance of reverting to the normal state from the superconductive state.
These and other objects will in part be obvious and will in part appear hereinafter.
The invention is now described with reference to the following description, taken in connection with the accompanying drawing.
The drawing consists of a single figure which is a schematic diagram of `a magnet constructed according to a preferred embodiment of the invention.
As shown in the drawing, the magnet comprises a soft iron core 10, including a movable pole piece 12 which may be moved into the position shown in dotted lines to form a closed magnetic loop. Currents are induced in the core by a copper coil 14 connected to a suitable power supply 16. The superconducting solenoid 18 comprises closed loops, which may be cylinders as shown in the drawing or closed loop wires. The cylinders can be made of formed and sintered NjbBSn powders or extruded Nb-Zr tubing. Non-superconductor cylinders should be provided to radially separate the superconductive cylinders. Copper is a preferred choice for this purpose. Where wire is used, it can be of the type described by Kunzler et al. in 6 Physical Review 89 (1961). However, the wires should be formed into closed loops before sintering.
The superconducting coil is held in a Dewar flask 20 of annular form which is placed around a pole piece of the core 10.
The operation of this magnet assembly begins with the pole piece 12 closing the air gap of the magnet and the temperature ofthe superconductive coil above the critical temperature of Iits constituent material. Power is supplied to the copper coil to induce a eld in the iron core up to its saturation limit. Then helium is supplied to the Dewar 20 to lower the temperature of the coil 18 below the critical temperature. So far, no current flows in the superconducting coil.
The copper coil is then cut off from the power supply. This causes -a small current to be induced in the superconducting coil, but the iron core remains saturated. Then the air gap is opened by lowering the pole piece 12. Additional current is induced in the .superconducting coil and the constant flow of current without resistance maintains the high field across the air gap. The field in the gap is maintained so long as the coil is kept at liquid helium temperature and the `air gap spacing is not too great. When the air gap spacing is excessive, the coil 18 will go normal. The current in the coils will cause a resistive heating which is dissipated by helium boil-off. The superconductive loops will not burn out.
It wil-l be appreciated by those skilled in -the art that the limits of the present invention are defined by the saturation field of the ferromagnetic core-about 25,000 gauss for iron. The diameters of the pole faces are unlimited.
It will also be appreciated by those skilled in the art that variations can be made Within the scope of the present invention. For instance, the pole piece 12 can be rigidly attached to the remainder of core 10 and the air gap lled by a removable iron keeper. The superconductive loops can be simple niobium cylinders or hard superconductor alloys made by the diffusion technique described by Saur in Die Naturwissenschaften, 49, p. 129 (1962). The location of the superconducting coil near a pole face, as shown in the drawing, is preferred to reduce stray flux when the air gap is opened. However, this location is not critical to the invention.
What is claimed is:
l. A superconducting magnet characterized by burnout proof protection for superconductive windings and freedom from relatively low critical current capacity section, such as joints, and comprising, in combination: a ferromagnetic core with a magnet gap, means for creating a magnetic field in the core, a superconducting coil electromagnetically linked to the ferromagnetic core, the coil comprising closed rings of superconducting material in an essentially closed space, a cryogenic fluid having a temperature below the critical temperature of the superconducting material, means for admitting said cryogenic iiuid to said space for lowering the temperature of the coil below the critic-al temperature of the superconducting material, a portion of said ferromagnetic core being movable relative to the rest of the core between at least a first position wherein the core has said magnet gap and a second position wherein said gap is closed, with said core portion providing a consistently large cross-section area for bridging the gap in said second position, and means connected to said core portion and constructed and arranged to move said core portion between said first and second positions, and closing the gap of the ferromagnetic core.
2. A superconducting magnet characterized by burnout proof protection for superconductive windings and freedom from relatively low critical current capacity section, such as joints, and comprising in combination: a closed loop ferromagnetic core, a superconducting coil electromagnetically linked to the ferromagnetic core, the coil comprising closed rings of superconducting material in an essentially closed space, a cryogenic uid having a temperature below the critical temperature of the superconducting material, means for admitting said cryogenic uid to said space for lowering the temperature of the coil below the critical temperature of the superconducting material, means forming a portion of said closed loop ferromagnetic core of consistently large cross-section area, said means being constructed and arranged so that it is removable from the core to leave a magnet gap in the core when it is removed.
References Cited by the Examiner UNITED STATES PATENTS 3,158,792 11/1964 Swartz et al. 317-158 BERNARD A. GILHEANY, Primary Examiner.
JOHN F. BURNS, Examiner.
GEORGE HARRIS, JR. Assistant Examiner.
Patented May 24, '1966
Claims (1)
1. A SUPERCONDUCTING MAGNET CHARACTERIZED BY BURNOUT PROOF PROTECTION FOR SUPERCONDUCTIVE WINDINGS AND FREEDOM FROM RELATIVELY LOW CRITICAL CURRENT CAPACITY SECTION, SUCH AS JOINT, AND COMPRISING, IN COMBINATION: A FERROMAGNETIC CORE WITH A MAGNET GAP, MEANS FOR CREATING A MAGNETIC FIELD IN THE CORE, A SUPERCONDUCTING COIL ELECTROMAGNETICALLY LINKED TO THE FERROMAGENTIC CORE, THE COIL COMPRISING CLOSED RINGS OF SUPERCONDUCTING MATERIAL IN AN ESSENTIALLY CLOSED SPACE, A CRYOGENIC FLUID HAVING A TEMPERATURE BELOW THE CRITICAL TEMPERATURE OF THE SUPERCONDUCTING MATERIAL, MEANS FOR ADMITTING SAID CRYOGENIC FLUID TO SAID SPACE FOR LOWERING THE TEMPERATURE OF THE COIL BELOW THE CRITICAL TEMPERATURE OF THE SUPERCONDUCTING MATERIAL, A PORTION OF SAID FERROMAGNETIC CORE BEING MOVABLE RELATIVE TO THE REST OF THE CORE BETWEEN AT LEAST A FIRST POSITION WHEREIN THE CORE HAD SAID MAGNET GAP AND A SECOND POSITION WHEREIN SAID GAP IS CLOSED, WITH SAID CORE PORTION PROVIDING A CONSISTENTLY LARGE CROSS-SECTION AREA FOR BRIDGING THE GAP IN SAID SECOND POSITION, AND MEANS CONNECTED TO SAID CORE PORTION AND CONSTRUCTED AND ARRANGED TO MOVE SAID CORE PORTION BETWEEN SAID FIRST AND SECOND POSITIONS, AND CLOSING THE GAP OF THE FERROMAGNETIC CORE.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US309986A US3253192A (en) | 1963-09-19 | 1963-09-19 | Superconducting solenoid apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US309986A US3253192A (en) | 1963-09-19 | 1963-09-19 | Superconducting solenoid apparatus |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| US3253192A true US3253192A (en) | 1966-05-24 |
Family
ID=23200506
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US309986A Expired - Lifetime US3253192A (en) | 1963-09-19 | 1963-09-19 | Superconducting solenoid apparatus |
Country Status (1)
| Country | Link |
|---|---|
| US (1) | US3253192A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3370258A (en) * | 1965-12-10 | 1968-02-20 | Gen Electric Co Ltd | Methods of and apparatus for the production of magnetic fields using superconductingmagnets |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3158792A (en) * | 1961-11-02 | 1964-11-24 | Gen Electric | Superconductive devices |
-
1963
- 1963-09-19 US US309986A patent/US3253192A/en not_active Expired - Lifetime
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3158792A (en) * | 1961-11-02 | 1964-11-24 | Gen Electric | Superconductive devices |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3370258A (en) * | 1965-12-10 | 1968-02-20 | Gen Electric Co Ltd | Methods of and apparatus for the production of magnetic fields using superconductingmagnets |
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