Superconductor technology: apparatus – material – process – High temperature devices – systems – apparatus – com- ponents,... – Superconductor layer next to free metal containing layer
Reexamination Certificate
2001-04-12
2003-07-01
Talbot, Brian K. (Department: 1762)
Superconductor technology: apparatus, material, process
High temperature devices, systems, apparatus, com- ponents,...
Superconductor layer next to free metal containing layer
C505S434000, C174S125100, C428S403000, C428S930000
Reexamination Certificate
active
06586370
ABSTRACT:
BACKGROUND OF THE INVENTION
1). Field of the Invention
The present invention relates to a superconductor.
2). Discussion of Related Art
The discovery of high critical temperature (Tc) superconducting ceramics (HTS ceramics) has inspired an enormous interest in their application. Conventional niobium alloy superconductors such as NbTi must be cooled to below 10K to achieve useful superconductivity. HTS superconductors, on the other hand, can have Tcs over 100K. Due to the great expense of cryogenic refrigeration, the HTS ceramics could find much wider application in industrial and laboratory devices. Of particular interest are materials which have Tc above 77K, because this is the temperature of liquid nitrogen, a common and relatively inexpensive refrigerant.
HTS ceramics have not been used in many potential applications because they suffer from a number of shortcomings. The most severe problems with the HTS ceramics are as follows:
1) HTS ceramics are brittle. They are not flexible and thus cannot be made into wires or other useful shapes. Cracks and boundaries between adjacent crystals severely limit supercurrent flow.
2) HTS ceramics are highly anisotropic. Supercurrents preferentially flow in certain directions with respect to the crystal lattice, reducing the maximum current density in randomly oriented multicrystalline pieces.
3) HTS ceramics are strong oxidizing agents. Most metals, such as copper, lead, tin, aluminum, indium and niobium, are oxidized by contact with the ceramic superconductors. Insulating oxide layers impede supercurrent flow. Only noble metals such as gold, silver palladium and their alloys are not oxidized by the HTS ceramics.
A less severe undesirable feature of the HTS ceramics is that they can lose their superconducting properties under certain circumstances. The superconducting structure inside the HTS ceramics has an abundance of oxygen atoms which are necessary for superconductivity. Heating, grinding, etching, or prolonged exposure to ambient atmosphere or vacuum may liberate the oxygen and destroy superconductivity. Both the oxygen content and the superconductivity can be restored by annealing the HTS ceramic in an atmosphere of oxygen.
It would be an advance in the art of applied superconductivity to provide a superconducting wire employing HTS ceramics that is ductile, has a high Tc, and has a high critical current density (Jc). Such a wire must overcome the problems with the HTS ceramics. Prior art HTS ceramic wires made of a combination of HTS ceramic particles in a silver matrix generally have poor superconducting properties such as low Jc. Also, bending the prior art wires tends to greatly reduce the Jc. This is highly undesirable.
There are other ceramic superconductor materials which have some of the same disadvantages as HTS cuprate materials. For example, the A15 family of superconductors such as Nb
3
Sn are also brittle materials (although they are not anisotropic and relatively nonreactive). Their poor mechanical properties have precluded their use in many applications requiring ductility such as wires. This is unfortunate because they generally have good superconducting properties such as relatively high Tcs, high critical magnetic fields, and high critical current densities.
Other examples of brittle, nonductile superconductors include materials possessing the NaCl crystal structure (the AB family), Laves phase ceramics, Chevrel phase ceramics and metallic borides. These materials may have superior superconducting properties, but are unusable in many applications (e.g., conducting wires) because they are brittle. It would be an advance in the art of applied superconductivity to provide flexible wires made from brittle superconductor materials.
U.S. Pat. No. 5,091,362 to Ferrando discloses a method for forming a silver coating on HTS ceramic particles. U.S. Pat. No. 4,971,944 to Charles et al. teaches a method for electroless deposition of gold onto HTS ceramic particles.
U.S. Pat. No. 5,041,416 to Wilson describes a superconducting composite material. Powders of HTS ceramic and normal metal are mixed and the mixture is subjected to heat and high pressure. The composite materials of Wilson have a relatively low Jc due to reactivity between the HTS ceramics and the metal matrix. The wires also have a low Jc if silver is used as the normal metal.
U.S. Pat. No. 5,202,307 to Hayashi describes a superconducting composite material having HTS ceramic particles in a metal matrix. The composite materials of Hayashi have a relatively low Jc due to reactivity between the HTS ceramic particles and the metal matrix and/or due to poor superconducting properties of the metal matrix materials.
U.S. Pat. No. 5,194,420 to Akihama describes a composite cuprate superconductor/metal superconducting material consisting of HTS ceramic particles dispersed in a matrix of silver. The composite materials of Akihama will also have a relatively low critical current density due to the choice of silver as the metal matrix material.
U.S. Pat. No. 5,081,072 to Hosokawa et al. describes a method preparing a HTS superconducting ceramic powder and forming the powder into a superconducting material. A low Jc is also a problem with the materials of Hosokawa.
U.S. Pat. No. 5,547,924 to Ito et al. describes a superconducting ceramic composite material having HTS ceramic particles in a noble metal matrix. The composite materials have relatively poor superconducting properties due to the poor superconducting properties of the metal matrix materials used.
U.S. Pat. No. 5,132,278 to Stevens et al. describes a cuprate superconductor wire having continuous filaments of HTS ceramic surrounded by metal matrix. A noble metal chemically protects the HTS ceramic. The wires of Stevens et al. are characterized in that they do not conduct current between wires, and do not rely on the superconducting proximity effect.
There exists a need for the HTS ceramic superconducting material that is ductile and has a high Jc that is not reduced by bending. Also, there exists a need for ductile superconducting materials made from brittle superconductors that have a high Jc high Tc, and high ductility.
SUMMARY OF THE INVENTION
The invention provides a superconductor comprising particles made of a planar diboride superconductive material, and a conductive material. The conductive material is selected to be driven to a superconductive state when in proximity to the superconductive material. An unbroken length of the conductive material is located sufficiently close to a plurality of the particles to be driven to a superconductive state by the superconductive material.
The planar diboride is preferably magnesium diboride.
The invention also provides a method of making such a superconductor. The invention also provides a method of making a wire of such a superconductor. An elongate member may be assembled from the particles and the conductive material, and be drawn into a wire.
REFERENCES:
patent: 4575927 (1986-03-01), Braginski et al.
patent: RE32178 (1986-06-01), Yoshizaki
patent: 4971944 (1990-11-01), Charles et al.
patent: 5091362 (1992-02-01), Ferrando
patent: 5248661 (1993-09-01), Mole et al.
patent: 5998336 (1999-12-01), Holcomb
patent: 54-97775 (1979-08-01), None
patent: 64-76960 (1989-03-01), None
patent: 03-275505 (1991-12-01), None
Blakely & Sokoloff, Taylor & Zafman
Nove' Technologies, Inc.
Talbot Brian K.
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