US3715451A - Superconductor structure, and method of making the same - Google Patents

Superconductor structure, and method of making the same Download PDF

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US3715451A
US3715451A US00180463A US3715451DA US3715451A US 3715451 A US3715451 A US 3715451A US 00180463 A US00180463 A US 00180463A US 3715451D A US3715451D A US 3715451DA US 3715451 A US3715451 A US 3715451A
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superconductor
sheath
metal
band
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C Levaire
A Hammer
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01BCABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
    • H01B12/00Superconductive or hyperconductive conductors, cables, or transmission lines
    • H01B12/16Superconductive or hyperconductive conductors, cables, or transmission lines characterised by cooling
    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

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  • An elongated metallic tube has secured therein, with substantial line contact, a sheathed filamentary superconductor, having an outside diameter much less than the inside diameter of the tube; preferably the sheath metal and the metal of the tube are the same (for example copper, aluminum, or alloys thereof).
  • a long band is provided along the length of which the superconductor is first bonded, for example by welding, or fusing of the sheath metal to the band; thereafter, the band is folded and formed into the tube, the lateral edges of the band being seamed together to form a fluid tight seal for example by welding, cold flowing or the like.
  • the present invention relates to superconductors, and to a method of making the same, and more particularly to superconductor structures of substantiallength with efficient cooling arrangement.
  • Superconductors are usually formed in sheets, tapes, or wires and it is difficult to make them in substantial length.
  • the superconductive materials themselves usually are intermetallic compounds containing niobi urn, tin, vanadium, such as Nb, Sn; Nb Al Nb Au; Nb Ti", V Si; V Ga.
  • the state of the superconductors is determined by their temperature and the magnetic field to which theyare exposed, and when both temperature and field are below a critical value they are in superconductive state.
  • the critical temperature and magnetic field values vary in accordance with the composition of the superconductor, and to a certain extent in accordance with their structure.
  • the critical magnetic fields are in the order of several tens to hundred thousands Oersteds.
  • the highest critical temperatures are in the range from to 18K.
  • the superconductors are usually maintained immersed in a refrigerating fluid, such as liquid helium.
  • a refrigerating fluid such as liquid helium.
  • the containers for refrigerating liquid are quite large and the auxiliary equipment for use with the superconductive structure is substantial. Entirely apart from the dimensions and mass of the auxiliary equipment, the cost of maintaining sufficient quantities of refrigerating liquid at low temperature is prohibitive for a large number of industrial applications.
  • soft superconductors When so called soft superconductors are cooled, they are usually made in tubular, or hollow form to permit this internal cooling; electrical connections necessary to apply the superconductors currents then are made to the surface of such elements. Even so called hard superconductors are frequently formed in hollow, or tubular form, a shape which permits great increase in the value of the critical magneticfield.
  • Superconductors for internal cooling have a central bore into which superconductive fluid is introduced under pressure, or under variable flow conditions. Yet, single elementarysuperconductor structures, such as supercondutor wires, may have only a small cross section and the resulting bore therethrough will be of insufficient size in order to permit sufficient flow for correct cooling.
  • Certain-multiple-element superconductors are better adapted for cooling by internal flow of cooling fluid.
  • Such superconductor structures may consist of a certain number of filamentary elements spaced from each other and surrounded by amass of metal stabilizing their thermal conduction, the hollow superconductors each having a bore of sufficient size adapted to receive refrigerating fluid. Nevertheless, such multiple-element superconductors have fair cooling capability although a substantial amount of refrigerating fluid is required. Additionally, under present manufacturing techniques, such superconductors can be made only in comparatively sort length.
  • a superconductor which may be hollow is surrounded by a metallic sheath; the sheathed superconductor, itself, is inserted into a tube of preferably the same metal as the sheath, and of substantially larger internal diameter than the external diameter of the sheathed superconductor.
  • the sheathed superconductor is connected by means of an essentially line-contact along the length of the tube. Refrigerating fluid is then introduced into the tube surrounding the superconductor.
  • the interconnection between the superconductor and the metal of the tube may be by welding, brazing or the like, and the superconductor itself, if desired, may be hollow.
  • the exterior surface of the superconductive element is in constant thermal contact with the refrigerating fluid; heat exchange is thus substantial since the surface of the superconductive element over which heat exchange may obtain is great with respect to the sur-' face ofan internal bore alone.
  • the superconductor structure is made by bonding (fusing, welding or the like) the sheathed superconductor to an elongated ribbon or tape of metal which is then folded over to be formed into the tube surrounding the superconductor the longitudinal edges of the tape or band being secured together to be fluid tight for example by hot or cold welding, cold flowing of the metal or the like. More than one sheathed superconductor may be applied longitudinally to the tape or ribbon, so that a structure with a number of superconductors secured along the length of the tube will be obtained.
  • FIG. 1 is a schematic cross-sectional view through a composite superconductor structure in accordance with the prior art, with the scale of the various elements arbitrarily chosen;
  • FIG. 2 is a cross-sectional transverse view, not to scale, of the superconductor structure in accordance with the present invention
  • FIG. 3 illustrates a step in the manufacture of the superconductor structure
  • FIG. 4 is a transverse cross-sectional view, to arbitrary scale of an alternate embodiment of the invention.
  • the body of metal has a central bore 2a which may be circular, polygonal, or of some other shape to pass cryogenic liquid therethrough.
  • the best possible heat exchange between the cryogenic liquid and the superconductor elements themselves cannot be realized in this manner and superconductor structures of substantial length are difficult to make.
  • The'cooling of superconductors of this type is achieved in the known manner by circulating a refrigerating fluid, under pressure, through bore 2a.
  • the superconductor is a filamentary element 3 supplied with a sleeve or sheath 4 of a stabilization metal, such as aluminum, copper, or alloys of aluminum or copper, or such other appropriate metal which it is a good thermal conductor at cryogenic temperatures.
  • a stabilization metal such as aluminum, copper, or alloys of aluminum or copper, or such other appropriate metal which it is a good thermal conductor at cryogenic temperatures.
  • the superconductor element 3 with its sheath 4 is secured along one side, with substantially line contact to the inner wall of a tube 5.
  • the superconductor element 3 maybe single elements, or multiple elements, and the tube 5 maybe of circular, or other cross section, so long as it is fluid tight so that cryogenic refrigerating liquid will not leak therefrom.
  • the superconductor'structure of the present invention is cooled by introducing refrigerating liquid, under pressure, into tube 5; the fluid introduced therein may have a controlled flow rate, to control the heat transfer available.
  • the refrigerating fluid is in contact with sheath 4 surrounding the superconductive element 3.
  • the heat exchange surface between superconductor element 3 and the refrigerating fluid is, consequently substantial and the path for heat flux across the sheath 4, between superconductor 3, and the surrounding refrigerating fluid, is of increasing heat carrying capability.
  • Extreme cooling rates can be obtained by making the superconductor element hollow, that is by forming a central bore 6 therein, and connecting additional refrigerating fluid to the central bore.
  • the superconductor just described is made by first sheathing the superconductor element 3 with a stabilization metal 4.
  • the sheathed composite element is then placed longitudinally on a tape, or ribbon, or band material 5a (see FIG. 3), and the metals of the sheath 4 and of band or tape 50 are fused together, for example, by welding, brazing or the like, so that an essentially line contact between thesuperconductor and the tape will be formed.
  • band 5a is bent or folded into tubular shape to form the cylinder 5 (which may have a round, polygonal or other cross section), the superconductor element 3 then being interior of tube 5.
  • the longitudinal edges 7, 8 of tape 5a are then joined to form a tight connection, for example by welding, cold flowing, brazing, fusing or similar method.
  • Both the welding of sheath 4 of the superconductor element on tape 5a, and welding together of the longitudinal edges 7,8, can be done by cold working the metal under substantial pressure; hot fusion, with or without addition of further metal may also be used.
  • Superconductor structures may thus be made of any length desired and having any desired dimensions. The resulting structure is form stable and can readil be cooled,
  • a plurality of superconductor elements 9 can be placed within a stabilization metal sleeve 10, each in turn laterally fused to the inner wall of a tube 11 (see FIG. 4).
  • Tube 11 itself can again be made from a flat tape, with the plurality of sheathed elements located lengthwise thereof, the tape then being folded and secured at its lateral edges as seen at 12, for example by welding, so that a fluid tight seal will result.
  • the tubular body may have a circular, polygonal, or other cross section.
  • the cross section of the tube 11, the number, and the dimensions of the superconductive elements 9 may be chosen in accordance with design requirements of the superconductor element itself, and as determined by the application for which it is to be used, the critical current, and the coefficient of stabilization, so that maximum cooling effect can be obtained with a minimum amount of refrigerating fluid being passed through the tube 11.
  • the dimensions, number of superconductive elements, and shapes can be varied to suit various design requirements.
  • Superconductive structure adapted to be cooled by a cryogenic fluid comprising:
  • a'fluid tight metallic tube (5) adapted to contain said cryogenic fluid

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Abstract

An elongated metallic tube has secured therein, with substantial line contact, a sheathed filamentary superconductor, having an outside diameter much less than the inside diameter of the tube; preferably the sheath metal and the metal of the tube are the same (for example copper, aluminum, or alloys thereof). According to the method, a long band is provided along the length of which the superconductor is first bonded, for example by welding, or fusing of the sheath metal to the band; thereafter, the band is folded and formed into the tube, the lateral edges of the band being seamed together to form a fluid tight seal for example by welding, cold flowing or the like.

Description

ited States Patent 1 1 Hammer et al.
[54] SUPERCONDUCTOR STRUCTURE,
AND METHOD OF MAKING THE SAME [76] Inventors: Alfred Paul Hammer, 107 Avenue Victor Hugo, Paris 16 eme; Alexis Charles Entz, 16, Alice du l-laras, 92 Vaucresson; Claude Levaire, 12, Place St. Momble, O2 Chauny, all of France 52 US. Cl. ..174/15C,174/27,174/126CP, 1 174/128, 174/010. 6, 335/216 51 11m. (:1. .1101117/34 [58] Field ofSearch ..174/15 (3, DIG. 6, 113 R, 113 AS, 174/126 R, 126 CP, 128, 28, 27
[56'] References Cited UNITED STATES PATENTS 7/1971 Kakfa ..l74/28 5/1970 Lawton ..l74/l5C 1 1 Feb. 6, 1973 Kafka ..1 74 15 0 Garwin ..174/l5 C OTHER PUBLICATIONS E. C. Rogers et 211., Design for a Superconducting A.C.
'Power Cable, Proc. lEEE, Vol. 118, No. 10, October [57] ABSTRACT An elongated metallic tube has secured therein, with substantial line contact, a sheathed filamentary superconductor, having an outside diameter much less than the inside diameter of the tube; preferably the sheath metal and the metal of the tube are the same (for example copper, aluminum, or alloys thereof). According to the method, a long band is provided along the length of which the superconductor is first bonded, for example by welding, or fusing of the sheath metal to the band; thereafter, the band is folded and formed into the tube, the lateral edges of the band being seamed together to form a fluid tight seal for example by welding, cold flowing or the like.
5 Claims, 4 Drawing Figures PATENTEDIFEB- slaw III-5 SUPERCONDUCTOR STRUCTURE, AND METHOD OFMAKING THE SAME This is adivision, of application Ser. No. 861,910 filed Sept. 29, I969 is now U.S. Pat. No. 3,626,585.
The present invention relates to superconductors, and to a method of making the same, and more particularly to superconductor structures of substantiallength with efficient cooling arrangement.
Superconductors are usually formed in sheets, tapes, or wires and it is difficult to make them in substantial length. The superconductive materials themselves usually are intermetallic compounds containing niobi urn, tin, vanadium, such as Nb, Sn; Nb Al Nb Au; Nb Ti", V Si; V Ga. The state of the superconductors is determined by their temperature and the magnetic field to which theyare exposed, and when both temperature and field are below a critical value they are in superconductive state. The critical temperature and magnetic field values vary in accordance with the composition of the superconductor, and to a certain extent in accordance with their structure. The critical magnetic fields are in the order of several tens to hundred thousands Oersteds. The highest critical temperatures are in the range from to 18K.
For high cooling, the superconductors are usually maintained immersed in a refrigerating fluid, such as liquid helium. As a result, the containers for refrigerating liquid are quite large and the auxiliary equipment for use with the superconductive structure is substantial. Entirely apart from the dimensions and mass of the auxiliary equipment, the cost of maintaining sufficient quantities of refrigerating liquid at low temperature is prohibitive for a large number of industrial applications. It has already been proposed to substitute for cooling by immersing, cooling of the superconductive structure by internally conducting a cooling fluid therethrough, similar to cooling of welding electrodes. When so called soft superconductors are cooled, they are usually made in tubular, or hollow form to permit this internal cooling; electrical connections necessary to apply the superconductors currents then are made to the surface of such elements. Even so called hard superconductors are frequently formed in hollow, or tubular form, a shape which permits great increase in the value of the critical magneticfield.
Superconductors for internal cooling have a central bore into which superconductive fluid is introduced under pressure, or under variable flow conditions. Yet, single elementarysuperconductor structures, such as supercondutor wires, may have only a small cross section and the resulting bore therethrough will be of insufficient size in order to permit sufficient flow for correct cooling.
Certain-multiple-element superconductors are better adapted for cooling by internal flow of cooling fluid. Such superconductor structuresmay consist of a certain number of filamentary elements spaced from each other and surrounded by amass of metal stabilizing their thermal conduction, the hollow superconductors each having a bore of sufficient size adapted to receive refrigerating fluid. Nevertheless, such multiple-element superconductors have fair cooling capability although a substantial amount of refrigerating fluid is required. Additionally, under present manufacturing techniques, such superconductors can be made only in comparatively sort length.
' superconductor structure, and a method of making the same, which enables efficient and optimum cooling throughout a substantial length.
SUBJECT MATTER or THE PRESENT INVENTION Briefly, a superconductor which may be hollow is surrounded by a metallic sheath; the sheathed superconductor, itself, is inserted into a tube of preferably the same metal as the sheath, and of substantially larger internal diameter than the external diameter of the sheathed superconductor. The sheathed superconductor is connected by means of an essentially line-contact along the length of the tube. Refrigerating fluid is then introduced into the tube surrounding the superconductor. The interconnection between the superconductor and the metal of the tube may be by welding, brazing or the like, and the superconductor itself, if desired, may be hollow.
The exterior surface of the superconductive element is in constant thermal contact with the refrigerating fluid; heat exchange is thus substantial since the surface of the superconductive element over which heat exchange may obtain is great with respect to the sur-' face ofan internal bore alone.
According to a feature of the invention, the superconductor structure is made by bonding (fusing, welding or the like) the sheathed superconductor to an elongated ribbon or tape of metal which is then folded over to be formed into the tube surrounding the superconductor the longitudinal edges of the tape or band being secured together to be fluid tight for example by hot or cold welding, cold flowing of the metal or the like. More than one sheathed superconductor may be applied longitudinally to the tape or ribbon, so that a structure with a number of superconductors secured along the length of the tube will be obtained.
IN THE ACCOMPANYING DRAWINGS FIG. 1 is a schematic cross-sectional view through a composite superconductor structure in accordance with the prior art, with the scale of the various elements arbitrarily chosen;
FIG. 2 is a cross-sectional transverse view, not to scale, of the superconductor structure in accordance with the present invention; 7
FIG. 3 illustrates a step in the manufacture of the superconductor structure;
FIG. 4 is a transverse cross-sectional view, to arbitrary scale of an alternate embodiment of the invention.
A superconductor structure of the type illustrated in FIG. 1, which is known, usually has a certain number of filamentary superconductor elements 1 surrounded by a metal stabilization mass 2, such as a body of aluminum copper, or similar metal which is a good thermal conductor at the cryogenic temperatures. The body of metal has a central bore 2a which may be circular, polygonal, or of some other shape to pass cryogenic liquid therethrough. The best possible heat exchange between the cryogenic liquid and the superconductor elements themselves cannot be realized in this manner and superconductor structures of substantial length are difficult to make. The'cooling of superconductors of this type is achieved in the known manner by circulating a refrigerating fluid, under pressure, through bore 2a. Due, primarily, to the quite small heat exchange surface of the internal wall of bore 2a, and the progressive decrease of the sectionof material available for heat transfer between superconductor elements and the central bore, the effectiveness of cooling is low and a large amountof refrigerating fluid must be circulated.
In accordance with the present invention, the superconductor, as seen in FIG. 2, is a filamentary element 3 supplied with a sleeve or sheath 4 of a stabilization metal, such as aluminum, copper, or alloys of aluminum or copper, or such other appropriate metal which it is a good thermal conductor at cryogenic temperatures. The superconductor element 3 with its sheath 4 is secured along one side, with substantially line contact to the inner wall of a tube 5. Tube 5, itself,
is made of a metal which can be operated at cryogenic temperatures, and further is compatible with the sheath 4 surrounding the superconductor element, preferably of the same metal as the sheath itself. The superconductor element 3 maybe single elements, or multiple elements, and the tube 5 maybe of circular, or other cross section, so long as it is fluid tight so that cryogenic refrigerating liquid will not leak therefrom.
The superconductor'structure of the present invention is cooled by introducing refrigerating liquid, under pressure, into tube 5; the fluid introduced therein may have a controlled flow rate, to control the heat transfer available. The refrigerating fluid is in contact with sheath 4 surrounding the superconductive element 3. The heat exchange surface between superconductor element 3 and the refrigerating fluidis, consequently substantial and the path for heat flux across the sheath 4, between superconductor 3, and the surrounding refrigerating fluid, is of increasing heat carrying capability. Extreme cooling rates can be obtained by making the superconductor element hollow, that is by forming a central bore 6 therein, and connecting additional refrigerating fluid to the central bore.
In accordance with the feature of the invention, the superconductor just described is made by first sheathing the superconductor element 3 with a stabilization metal 4. The sheathed composite element is then placed longitudinally on a tape, or ribbon, or band material 5a (see FIG. 3), and the metals of the sheath 4 and of band or tape 50 are fused together, for example, by welding, brazing or the like, so that an essentially line contact between thesuperconductor and the tape will be formed. Thereafterband 5a is bent or folded into tubular shape to form the cylinder 5 (which may have a round, polygonal or other cross section), the superconductor element 3 then being interior of tube 5. The longitudinal edges 7, 8 of tape 5a are then joined to form a tight connection, for example by welding, cold flowing, brazing, fusing or similar method. Both the welding of sheath 4 of the superconductor element on tape 5a, and welding together of the longitudinal edges 7,8, can be done by cold working the metal under substantial pressure; hot fusion, with or without addition of further metal may also be used. Superconductor structures may thus be made of any length desired and having any desired dimensions. The resulting structure is form stable and can readil be cooled,
In accordance with a fea ure of the invention, a plurality of superconductor elements 9 can be placed within a stabilization metal sleeve 10, each in turn laterally fused to the inner wall of a tube 11 (see FIG. 4). Tube 11 itself can again be made from a flat tape, with the plurality of sheathed elements located lengthwise thereof, the tape then being folded and secured at its lateral edges as seen at 12, for example by welding, so that a fluid tight seal will result. Again, the tubular body may have a circular, polygonal, or other cross section.
The cross section of the tube 11, the number, and the dimensions of the superconductive elements 9 may be chosen in accordance with design requirements of the superconductor element itself, and as determined by the application for which it is to be used, the critical current, and the coefficient of stabilization, so that maximum cooling effect can be obtained with a minimum amount of refrigerating fluid being passed through the tube 11.
The dimensions, number of superconductive elements, and shapes can be varied to suit various design requirements.
We claim:
1. Superconductive structure adapted to be cooled by a cryogenic fluid comprising:
a'fluid tight metallic tube (5) adapted to contain said cryogenic fluid;
a filamentary superconductor (3) located in said tube;
a metallic sheath (4) surrounding said superconductor, said sheath (4) being secured with a substantially line contact to the inside wall of said tube and having a lesser outside diameter than the in side diameter of said tube.
2. Superconductive structure according to claim 1, wherein a plurality (FIG. 4) of superconductors, each surrounded by a sheath, are located in said tube, the sheaths of said superconductors being secured with substantially even spacing to the inside wall of said tube.
3. Superconductive structure according to claim 1, wherein the metal of said sheath and of the tube are alike.
4. Superconductive structure, according to claim 1, wherein the metal of the sheath and of the tube are aluminum, or copper, or alloys thereof.
5. Superconductive structure according to claim 1, wherein the filamentary superconductor has a longitudinally extending bore (6) therein for connection to a source ofcryogenic fluid.
Patent No EDWARD M.FLETCHER.,JR.
5,715,451 Dated, F r y 97.3
Inventofls) ALFRED PAUL HAMMER, ET.- EAL.
It is certified that error agp ears in the above-identified patent and that said Letters Patent are hereby corrected as shown below:
On the cover sheet, insert [30] Claims Foreign Priority Dam France October 18, 1968, 'No..'170,4l5
On the oover sheet, insert [73] Assigne (jompagnie Francaise Thomson Houston-Hofchkiss Brandt Paris, France Signed and sealed this 22nd day oiiJannery 1974.
( SEAL) Attest:
RENE D. TEGTMEYER Attesting Officer Acting Commissioner of Patents Imam."-
UNITED STATES PATENT OFFICE QERTIFICATE OF CORRECTION Patent No. 3,715,451 Dated February 6, 197 3 inventor ALFRED PAUL HAMMER, ET. CAL.
It is certified that error appears in the above-identified patent and that said Letters Patent are hereby corrected as shown below:
On the cover sheet, insert [30] Claims Foreign Priority Data France October 18, 1968, 'No.-l70,4l5
On the cover sheet; insert [73] Assignee-Compagnie Francaise Thomson Houston-Hotchkiss Brandt Paris, France Signed and sealed this 22nd day of Jannery 1974.
(SEAL) Attest: A
EDWARD M.PLETCHER,JR. Q RENE D. TEGTMEYER Attesting Officer 7 Acting Commissioner of Patents

Claims (5)

1. Superconductive structure adapted to be cooled by a cryogenic fluid comprising: a fluid tight metallic tube (5) adapted to contain said cryogenic fluid; a filamentary superconductor (3) located in said tube; a metallic sheath (4) surrounding said superconductor, said sheath (4) being secured with a substantially line contact to the inside wall of said tube and having a lesser outside diameter than the inside diameter of said tube.
1. Superconductive structure adapted to be cooled by a cryogenic fluid comprising: a fluid tight metallic tube (5) adapted to contain said cryogenic fluid; a filamentary superconductor (3) located in said tube; a metallic sheath (4) surrounding said superconductor, said sheath (4) being secured with a substantially line contact to the inside wall of said tube and having a lesser outside diameter than the inside diameter of said tube.
2. Superconductive structure according to claim 1, wherein a plurality (FIG. 4) of superconductors, each surrounded by a sheath, are located in said tube, the sheaths of said superconductors being secured with substantially even spacing to the inside wall of said tube.
3. Superconductive structure according to claim 1, wherein the metal of said sheath and of the tube are alike.
4. Superconductive structure, according to claim 1, wherein the metal of the sheath and of the tube are aluminum, or copper, or alloys thereof.
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Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5114908A (en) * 1989-08-09 1992-05-19 Sumitomo Electric Industries, Ltd. Superconductive conductor
US6525265B1 (en) * 1997-11-28 2003-02-25 Asea Brown Boveri Ab High voltage power cable termination
US6576843B1 (en) 2000-07-17 2003-06-10 Brookhaven Science Associates, Llc Power superconducting power transmission cable

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3343035A (en) * 1963-03-08 1967-09-19 Ibm Superconducting electrical power transmission systems
US3512581A (en) * 1967-07-03 1970-05-19 British Insulated Callenders Cryogenic devices
US3529071A (en) * 1967-04-29 1970-09-15 Siemens Ag Superconducting cable for transmitting high electrical currents
US3595982A (en) * 1967-12-20 1971-07-27 Siemens Ag Supercounducting alternating current cable

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3343035A (en) * 1963-03-08 1967-09-19 Ibm Superconducting electrical power transmission systems
US3529071A (en) * 1967-04-29 1970-09-15 Siemens Ag Superconducting cable for transmitting high electrical currents
US3512581A (en) * 1967-07-03 1970-05-19 British Insulated Callenders Cryogenic devices
US3595982A (en) * 1967-12-20 1971-07-27 Siemens Ag Supercounducting alternating current cable

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
E. C. Rogers et al., Design for a Superconducting A.C. Power Cable, Proc. IEEE, Vol. 118, No. 10, October 1971 *

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5114908A (en) * 1989-08-09 1992-05-19 Sumitomo Electric Industries, Ltd. Superconductive conductor
US6525265B1 (en) * 1997-11-28 2003-02-25 Asea Brown Boveri Ab High voltage power cable termination
US6576843B1 (en) 2000-07-17 2003-06-10 Brookhaven Science Associates, Llc Power superconducting power transmission cable

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