Oxide superconducting wire

Abstract: An oxide superconducting wire of an anisotropic oxide superconductor comprises a core part of the wire and a superconducting layer enclosing the core part so that specific crystal axes of the oxide superconductor are oriented toward the core part. A method of producing a wire of an anisotropic oxide superconductor comprises the steps of arranging a metal sheath around a metal rod for forming a core part of the wire and charging powder of the oxide superconductor in a clearance between the metal sheath and the metal rod for preparing a composite material, and plastically working the composite material so that the metal sheath is larger in reduction of area than the metal rod.

Description: The present invention relates to a superconducting wire, and more particularly, it relates to a superconducting wire which is prepared from an oxide superconductor, and to a method for producing it. It has recently been reported that a composite oxide sintered body superconducts at a high critical temperature, and an attempt has been made to develop a superconductivity technique through such a superconductor. It has been reported that a YBaCuO oxide exhibits superconductivity at 90 K and BiPbSrCaCuO oxide exhibits superconductivity at 110 K. Such an oxide superconductor exhibits super conductivity in liquid nitrogen, which can be easily obtained at a relatively low cost, and hence the same is expected for practical use. In order to apply the oxide superconductor to the wire of a superconducting magnet, for example, it is necessary to work the same into a wire. However, It is known that such an oxide superconductor is anisotropic, and hence the crystals thereof must be oriented in a specific direction in or der to attain high critical current density (J c ). In general, powder of the oxide superconductor is charged in a metal sheath, drawn into a wire having a prescribed diameter, and thereafter worked by rolling or pressing to obtain a tape-type wire, in which crystals of the oxide superconductor are oriented in a prescribed direction. Proceedings of the 38th Electronics Components Conference, 9th - 11th May 1988, pages 176-180 discloses a superconducting ceramic composit wire missing an outer carrying metal layer. Japanese Journal of Applied Physics, Vol. 26, No. 10, October 1987, pages 1653-1656 discloses an Y-Ba-Cu oxide superconducting wire having no metal core part. Fig. 10 discloses a multicored wire. The Journal of the American Ceramic Society, Vol. 70, No. 12, C-388 - C-390 (1987) is directed to methods of producing superconducting wires. The influence on the texture of Y-Ba-Cu-O due to the application of extrusion or drawing or other working operations is shown in set publication. EP 0 380 115 B1, forming the basis of the preamble of claim 1, an oxide superconducting wire having an oxide superconductor between a metal core member and an outer covering metal sheath member is known. The c-axis of said oxide superconductor is radially oriented toward said core member. From DE 26 43 026 C2 and from DE 22 54 778 A a superconductor cable with a plurality of filaments of the metal-type is known. Between the filaments high resistivity layers are provived in order to reduce electric losses due to eddy currents. According to the present invention, the oxide superconducting layer provided around the central part is divided into a plurality of layers so as to increase boundaries between the oxide superconductor and a matrix as well as to increase pinning points, thereby improving pinning force. According to this aspect, the oxide superconducting layers are brought into configurations elongated along the circumferential direction as compared with the radial direction. In the worklng step, therefore, force is applied to the oxide superconducting layers perpendicularly to the circumferential direction, whereby the oxide superconducting layers are oriented along the longitudinal direction to facilitate flow of the current. According to this aspect, preferably, high-resistance layers of a material having high electrical resistance are interposed between the plurality of oxide superconducting layers. When an alternating current is fed, a coupled current flows through a matrix layer provided between each adjacent pair of oxide superconducting layers. This coupled current results in a loss when carrying ac. In order to reduce such a loss, therefore, it is necessary to minimize the coupled current. According to this preferred embodiment, the high resistance layers of the material having high electrical resistance are interposed between the plurality of oxide superconducting layers to reduce the coupled current, thereby reducing the loss caused when carrying ac. The material for the high-resistance layers may be prepared from a metal, ceramic or the like. When the matrix metal is prepared from silver, for example, a silver alloy or stainless steel may be employed as the material for the high-resistance layers. Such a material can also improve the strength of the matrix. However, the oxide superconductor has such anisotropy that its critical current density is extremely varied with the direction of an applied magnetic field. Thus, it is known that critical current density is significantly varied with a magnetic field which is applied in parallel to the tape surface and that applied perpendicularly to the tape surface in a tape-type wire of an oxide superconductor whose crystals are oriented in a prescribed direction. For example, the wire exhibits critical current density of about 1000 A/cm 2 when a magnetic field of 1 T is applied in parallel to the tape surface, while the current hardly flows in the case of a perpendicular magnetic field. When such a conventional tape-type wire is coiled to provide a superconducting magnet, the generated magnetic field is applied in different directions depending on a location of a wire portion in the coil, to cause difference in critical current density within the wire. The critical current density of the overall wire is dominated by portions having lower critical current density. Thus, it is impossible to attain high critical current density as a whole. It is known that a magnetic flux enters the interior of an oxide superconductor before the superconductor goes into an ordinary conducting state. This magnetic flux is unmovably fixed by "pinning", and it is necessary to improve such pinning force in order to attain high critical current density. However, no contrivance has been made to improve the pinning force In the prior art oxide superconduding wire, and hence it has been impossible to attain high critical density. A principal object of the present invention is to provide an oxide superconducting wire which can regularly keep constant critical current density regardless of the direction of application of a magnetic field, and a method of producing the same. Another object of the present Invention is to provide a superconducting wire having higher critical current density by improving pinning force. The present invention provides a wire of an anisotropic oxide superconductor, which comprises an oxide superconductingm oxide layer being divided into a plurality of layers and provided in configurations elongated in the circumferential direction as compared with the radial direction being characterised In that high-resistance layers of a material having high electrical resistance are provided around the superconducting layers. According to the present invention, the anisotropic oxide superconductor is not particularly restricted but may be prepared from a BiPbSrCaCuO oxide or a YBaCuO oxide, for example. The present invention is applicable to most of oxide superconductors since most of oxide superconducting wires are considered anisotropic in view of current flowability etc. A method of producing a superconducting wire comprises the steps of arranging around a metal core part rod a metal sheath and charging calcined and pulverised oxide powder in the clearance between said metal rod and said metal sheath for preparing a composite material and plastically working said composite material so that said metal sheath is larger in reducting of area than said metal rod. In order to plastically work the composite material so that the metal sheath is larger in reducting of area than the metal rod, the metal sheath and the metal rod are prepared from materials which are different in workability from each other, for example. In other words, the metal rod is prepared from an relatively unworkable metal, and the metal sheath is prepared from a relatively workable metal. Due tu such selection of the materials, it is possible to make higher reduction of area of the metal rod while making lower that of the metal sheath. When the oxide superconductor is prepared from a BiPbSrCaCuO oxide, for example, the metal sheath is formed of Ag, which is unreactive with the oxide superconductor, and the metal rod is formed of a metal such as Ni, for example, which is inferior in workability of Ag. In this case, the surface of the metal rod is preferably covered with Ag or the like, so that Ni is not reactively in contact with the oxide superconductor. The metal rod and the metal sheath may be prepared from the same metal while devising the method of plastic working so that the metal sheath is larger in reduction of area than the metal rod. The plastic working method is not particularly restricted in the present invention, while wire drawing, rolling or swaging may be employed. According to the present invention, the superconducting wire may have one or more core parts. A plurality of core parts may be provided In multi-core structure such as that of a conventional metallic superconducting wire. According to the inventive oxide superconducting wire, a superconducting layer is provided around the core part so that specific crystal axes of the oxide superconductor are oriented toward the core part. Therefore, the superconducting layer contains such crystals of the oxide superconductor that specific crystal axes are oriented in directions which are different by 360° from each other. Thus, any portion of the superconducting layer necessarily contains crystals of the oxide superconductor which exhibit the highest critical current density with respect to the applied magnetic field. In the inventive oxide superconducting wire, therefore, portions having high critical current density regularly exist in series along the longitudinal direction of the wire even if the magnetic field is partially applied in different directions. Thus, high critical current density can be maintained as a whole. The composite material is so plastically worked that the metal sheath is higher in reduction of area than the metal rod. Due to such plastic working, a clearance between the metal sheath and the metal rod is gradually reduced in thickness to compress the powder of the oxide superconductor which is charged in this clearance. Through such compression, the powder of the oxide superconductor is subjected to force which is similar to that for the conventional tape-type wire, and oriented in a prescribed direction. For example, an oxide superconductor which is prepared from a SiPbSrCaCuO oxide is cloven along the c-plane, and hence the c-axes, which are perpendicular to the c-plane, are oriented toward the core part. The BiPbSrCaCuO oxide superconductor has the highest critical current density along the direction of the c-plane, and the wire is so produced as to orient the oxide superconductor in this direction. As hereinabove described, the superconducting layer is so formed as to orient the c-axes toward the core part in the radial section of the wire, which is necessarily provided with portions having the highest critical current density with respect to any direction of application of the magnetic field. Thus, the portions having the highest critical current density are adapted to transport the current in the high magnetic field, to regularly ensure high critical current density regardless of the direction of the applied magnetic field. The inventive superconducting wire has no dependency on the direction of application of the magnetic field, but exhibits high critical current density with respect to any direction. A superconducting wire exhibiting high critical current density can be produced through simple steps in high productivity. The inventive oxide superconducting wire having the aforementioned advantages is usefully employed under a strong magnetic field particularly for a super conducting magnet having complicated field distribution. These and other objects, features, aspects and advantages of the present invention will become more apparent from the following detailed description of the present invention when taken in conjunction with the accompanying drawings. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a sectional view showing a preferred mode of the present invention; Fig. 2 is a sectional view showing Example according to the preferred mode of the present invention; and Fig. 3 is a sectional view showing a conventional superconducting wire prepared as reference example. DESCRIPTION OF THE PREFERRED EMBODIMENTS Example 1 Fig. 1 is a sectional view showing a preferred mode of the present invention. Referring to Fig. 1. a plurality of oxide superconducting layers 12 are dividedly provided around a central part. High-resistance layers 13 are provided around the oxide superconducting layers 12. Such high-resistance layers 13 are interposed between a matrix 11 and the oxide superconducting layers 12. Thus, the high-resistance layers 13 are necessarily interposed between adjacent pairs of the oxide superconducting layers 12, to increase electrical resistance therebetween and to reduce the coupled current which is caused when carrying ac. Example 2 Example according to the aforementioned preferred mode is now described. Powder materials of Bi 2 O 3 , PbO, SrCO 3 , CaCO 3 and CuO of not more than 1 µm in particle size were mixed with each other so that Si, Pb, Sr, Ca and Cu were in the ratios 1.8:0.4:2:2.2:3. This mixture was calcined twice at 800°C, sintered at 860°C, and then pulverized to obtain powder. This powder was charged in a silver pipe of 10 mm in inner diameter and 12 mm in outer diameter, and drawn into a wire of 4 mm in diameter. This wire was inserted in a silver palladium alloy pipe of 4 mm in inner diameter and 5 mm in outer diameter, and worked into a rectangular wire having a sectional curvature. The silver-palladium alloy pipe was adapted to form high-resistance layers in the finial superconducting wire. The rectangular wire was inserted in a silver pipe of mm in inner diameter and 8 mm in outer diameter, while a silver rod was inserted in its center. This substance was wire-drawn to a diameter of 3 mm, sintered at 345°C for 50 to 200 hours, further wire-drawn to a diameter of 1.5 mm and again sintered at 845°C for 50 hours. Fig.2 is a sectional view showing the wire thus obtained. As shown in Fig. 2, the silver rod formed a central part 25 at the center of the wire, while five sectorial rectangular wires 24 were provided around the central part 25. Oxide superconducting layers 21 were located within the sectorial rectangular wires 24, while matrix layers 22, which were formed from the silver sheath, were located around the oxide superconducting layers 21. High-resistance layers 23 were formed from the silver-palladium alloy sheath around the matrix layers 22. Six second sectorial rectangular wires were arranged to enclose the first sectorial rectangular wires 24, while an outermost layer 26 of a silver sheath was provided around the second sectorial rectangular wires. Fig. 3 shows a conventional superconducting wire which was prepared as reference example. Referring to Fig.3, a central part was formed by an oxide superconductor 31, which was enclosed by a silver sheath 32. Such a conventional wire was drawn into a diameter of 3 mm, subjected to heat treatment similarly to the above, Example, and again subjected to wire drawing. The wire drawing step was so carried out that the sectional area of the superconductor 31 was equal to the total sectional area of the oxide superconducting layers 21 shown in Fig. 2.Consequently, the diameter was 1.5 mm. Critical current density values of Example2 and the reference example were measured at a temperature of 77.3 K. The wire according to Example 2 exhibited critical current density of 8000 to 14000 A/cm 2 , while the reference example exhibited critical current density of about 1000 A/cm 2 . Alternating currents of 60 Hz were fed to these wires to measure ac losses. The wire according to Example 2 exhibited an ac loss of about ten to scores of percent as compared with the reference example. Thus, it has been confirmed that the inventive wire exhibited a smaller loss when carrying ac. According to this mode, as hereinabove described, the oxide superconducting layer for enclosing the central part is divided into a plurality of layers along the longitudinal direction, whereby the interfaces between the matrix layers and the oxide superconducting layers as well as the pinning points are increased to improve pinning force. Thus, the superconducting wire according to this mode exhibits higher critical current density as compared with the conventional wire. According to the present invention, as hereinabove described with reference to Example2, the high-resistance layers are interposed between the oxide superconducting layers so as to reduce the coupled current flowing between the oxide superconducting layers. Thus, it is possible to reduce the loss caused when carrying ac. Since the oxide superconducting layers are provided around the central part in the superconducting wire according to this Example, it is possible to apply compression stress to the oxide superconducting layers in plastic working of the wire to orient the crystals of the oxide superconductor in a direction for facilitating the flow of the current by preparing the central part from a material which is unworkable as compared with the material for the oxide superconducting layers. Thus, the critical current density can be further increased.

Claims: An oxide superconducting wire of an anisotropic oxide superconductor, comprising: a metal core part (25) of said wire, a superconductor oxide layer (12, 21 ) enclosing said metal core part (25) the c-axis of said superconducting oxide layer being radially oriented toward said core part (25), and an outer covering metal sheath layer (11, 26), characterized in that the superconducting oxide layer (12,21) being divided into a plurality of layers and provided in configurations elongated in the circumferential direction as compared with the radial direction, and that high resistance layers (13,23) of a material having a high electrical resistance are provided around the superconducting layers (12,21). An oxide superconducting wire according to claim 1, characterized in that each superconducting oxide layer (21) is enclosed with a metal matrix (22) between the superconducting oxide layer (21) and the high resistance layer (23).

Inventors: HIKATA TAKESHI, MUKAI HIDEHITO, SATO KENICHI, HIKATA, TAKESHI, MUKAI, HIDEHITO, SATO, KENICHI, HIKATA, TAKESHI, C/O OSAKA WORKS OF, MUKAI, HIDEHITO, C/O OSAKA WORKS OF, SATO, KENICHI, C/O OSAKA WORKS OF
Applicants: SUMITOMO ELECTRIC INDUSTRIES, SUMITOMO ELECTRIC INDUSTRIES, LTD.
Application year: 1990
Main classification: H01L39
IPC codes: C04B35, H01L39