Method for making Y123 superconducting material

Abstract

A superconducting material includes YBa.sub.2Cu.sub.3O.sub.7-δ and a nano-structured, preferably nanowires, WO.sub.3 dopant in a range of from 0.01 to 3.0 wt. %, preferably 0.075 to 0.2 wt. %, based on total material weight. Methods of making the superconductor may preferably avoid solvents and pursue solid-state synthesis employing Y, Ba, and/or Cu oxides and/or carbonates.

Claims

1. A method of synthesizing a superconducting material, comprising: heating an oxidized form of yttrium, an oxidized form of barium, and an oxidized form of copper in molar ratios of 1 (Y): 1.9 to 2.1 (Ba): 2.9 to 3.1 (Cu) in a range of from 850 to 1050° C. for a time in a range of from 8 to 16 hours, to obtain a Y-123; grinding a mixture comprising the Y-123 and 0.01 to 3.0 wt. %, relative to total mass of the mixture, of nano-structured WO.sub.3 to form a superconductor precursor; pressing the superconductor precursor at a pressure in a range of from 500 to 1000 MPa into a pre-sintered precursor; sintering the pre-sintered precursor at a temperature in a range of from 900 to 1000° C. for a period in a range of from 4 to 12 hours, to obtain a sintered product; and cooling the sintered product at a rate in a range of from 1 to 10° C./minute to obtain the superconducting material; wherein the superconducting material, comprises: a YBa.sub.2Cu.sub.3O.sub.7-δ matrix phase; and 0.05 to 0.2 wt. %, based on total superconductor weight, of particles of a dopant, wherein the dopant is the nano-structured WO.sub.3 in the form of WO.sub.3 nanowires and wherein the WO.sub.3 nanowires are disposed within voids between grain boundaries of the YBa.sub.2Cu.sub.3O.sub.7-δ matrix phase.

2. The method of claim 1, wherein the WO.sub.3 nanowires are present in the superconducting material in a range of from 0.075 to 0.2 wt. %.

3. The method of claim 1, further comprising: compressing the oxidized forms of yttrium, barium, and copper prior to the heating.

4. The method of claim 1, wherein the sintering is conducted in an atmosphere comprising air.

5. The method of claim 1, wherein the superconducting material has at least 97% YBa.sub.2Cu.sub.3O.sub.7-δ phase with orthorhombic crystal structure and Pmmm symmetry.

6. The method of claim 1, wherein the superconducting material comprises: no more than 0.5% of Y.sub.2BaCuO.sub.5 (Y-211); no more than 0.5% of YBaCu.sub.2O.sub.5-δ (Y-112); no more than 0.5% of YBa.sub.2Cu.sub.4O.sub.y (Y-124); no more than 0.5% of Y.sub.2Ba.sub.4Cu.sub.7O.sub.y (Y-247); and no more than 0.5% of BaCuO.sub.2, based on the total phases concentration.

7. The method of claim 1, wherein the superconducting material comprises no more than 1% of any further phases of YBCO than Y-123, based on the total phases concentration.

8. The method of claim 1, wherein the superconducting material has in its matrix a regular form of nanometer scale entities bright in contrast dispersed into grains.

9. The method of claim 1, wherein the superconducting material has a superconducting transition in a range of from 80 to 100 K.

10. The method of claim 1, wherein the superconducting material has a critical current density (J.sub.cm) in a range of from 1.0×10.sup.4 to 1.4×10.sup.4 A/cm.sup.2, in an applied magnetic field of 0 Tesla.

11. The method of claim 1, wherein the superconducting material has a critical current density (J.sub.cm) in a range of from 600 to 800 A/cm.sup.2, in an applied magnetic field of 1 Tesla.

12. The method of claim 1, wherein the superconducting material has a critical current density of at least 4×10.sup.3 to 10.sup.5 A/cm.sup.2 across a temperature range of from 60 to 10 K under a magnetic field in a range of from 0 to 6 Tesla.

13. A method of synthesizing a superconducting material, comprising: heating an oxidized form of yttrium, an oxidized form of barium, and an oxidized form of copper in molar ratios of 1 (Y): 1.9 to 2.1 (Ba): 2.9 to 3.1 (Cu) in a range of from 850 to 1050° C. for a time in a range of from 8 to 16 hours, to obtain a Y-123; grinding a mixture comprising the Y-123 and 0.01 to 3.0 wt. %, relative to total mass of the mixture, of nano-structured WO.sub.3 to form a superconductor precursor; pressing the superconductor precursor at a pressure in a range of from 500 to 1000 MPa into a pre-sintered precursor; sintering the pre-sintered precursor at a temperature in a range of from 900 to 1000° C. for a period in a range of from 4 to 12 hours, to obtain a sintered product; and cooling the sintered product at a rate in a range of from 1 to 10° C./minute to obtain the superconducting material; wherein the WO.sub.3 nanowires are present in the superconducting material in a range of from 0.075 to 0.2 wt. % based on total superconductor weight.

14. The method of claim 13, further comprising: compressing the oxidized forms of yttrium, barium, and copper prior to the heating.

15. The method of claim 13, wherein the sintering is conducted in an atmosphere comprising air.

16. The method of claim 13, wherein the superconducting material has at least 97% YBa.sub.2Cu.sub.3O.sub.7-δ phase with orthorhombic crystal structure and Pmmm symmetry.

17. The method of claim 13, wherein the superconducting material comprises: no more than 0.5% of Y.sub.2BaCuO.sub.5 (Y-211); no more than 0.5% of YBaCu.sub.2O.sub.5-δ (Y-112); no more than 0.5% of YBa.sub.2Cu.sub.4O.sub.y (Y-124); no more than 0.5% of Y.sub.2Ba.sub.4Cu.sub.7O.sub.y (Y-247); and no more than 0.5% of BaCuO.sub.2, based on the total phases concentration.

18. The method of claim 13, wherein the superconducting material comprises no more than 1% of any further phases of YBCO than Y-123, based on the total phases concentration.

19. The method of claim 13, wherein the superconducting material has in its matrix a regular form of nanometer scale entities bright in contrast dispersed into grains.

20. The method of claim 13, wherein the superconducting material has a superconducting transition in a range of from 80 to 100 K.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) A more complete appreciation of the invention and many of the attendant advantages thereof will be readily obtained as the same becomes better understood by reference to the following detailed description when considered in connection with the accompanying drawings, wherein:

(2) FIG. 1 shows X-ray powder diffraction (XRD) patterns of tungsten oxide (WO.sub.3) nanowires added YBa.sub.2Cu.sub.3O.sub.y (Y-123) products;

(3) FIG. 2A shows a scanning electron microscope image of WO.sub.3 nanowires added to a YBCO sample;

(4) FIG. 2B shows a scanning electron microscope image of WO.sub.3 nanowires added to a YBCO sample;

(5) FIG. 3A shows a plot of electrical resistivity versus temperature for Y-123 samples synthesized with different amounts of WO.sub.3 nanowires;

(6) FIG. 3B shows a plot of electrical resistivity versus temperature for Y-123 samples synthesized with different amounts of WO.sub.3 nanowires;

(7) FIG. 4 shows plots of hysteresis magnetization loops measured at 77 K of the products synthesized with amounts of WO.sub.3 nanowires varying between 0.0 to 0.2 wt. %;

(8) FIG. 5A shows plots of magnetization critical current density (J.sub.cm) versus magnetic field estimated from M vs. H hysteresis loops at 77 K for pristine and WO.sub.3 nanowires-added Y-123 samples;

(9) FIG. 5B shows plots of magnetic field dependence of the flux pinning force density at 77 K for pristine and WO.sub.3 nanowires-added Y-123 samples;

(10) FIG. 6A shows variation of J.sub.cm value at an applied magnetic field of 0 Tesla for a Y-123 sample sintered with various amounts of WO.sub.3 nanowires;

(11) FIG. 6B shows variation of J.sub.cm value at an applied magnetic field of 1 Tesla for a Y-123 sample sintered with various amounts of WO.sub.3 nanowires;

(12) FIG. 7A shows plots of critical current density J.sub.cm calculated from the M vs H loops at various temperatures for undoped Y-123 sample;

(13) FIG. 7B shows plots of critical current density J.sub.cm calculated from the M vs H loops at various temperatures for 0.1 wt. % WO.sub.3 nanowires-added Y-123 sample; and

(14) FIG. 8 shows plots of temperature dependence of the ratio of J.sub.cm between that of 0.1 wt. % WO.sub.3 nanowires added Y-123 and of non-added Y-123, R, at an applied magnetic field of 0 and 1 Tesla.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

(15) Aspects of the invention provide superconducting materials, comprising YBCO materials such as YBa.sub.2Cu.sub.3O.sub.7-δ (Y-123) and a nano-structured tungsten oxide dopant such as WO.sub.3 in a range of from 0.01 to 3.0 wt. %, based on total material weight. Herein, “superconductor” and “superconducting material” is treated identically and interchangeably, typically using “superconductor(s)” for brevity. The superconductor itself is not a nanostructure, and may be an amorphous or partially crystalline matrix, containing nano-structured WO.sub.3.

(16) Aspects of the invention provide methods of synthesizing a superconductor, comprising: heating an oxidized form of yttrium, an oxidized form of barium, and an oxidized form of copper in molar ratios of 1 (Y): 1.9 to 2.1 (Ba): 2.9 to 3.1 (Cu) in a range of from 850 to 1050, 900 to 1000, or 925 to 975° C. for a time in a range of from 8 to 16, 10 to 14, or 11 to 13 hours, to obtain a Y-123; grinding the Y-123 with 0.01 to 3.0, 0.02 to 1.0, 0.03 to 0.5, 0.05 to 0.2 wt. %, relative to total superconductor mass, of WO.sub.3 nano-structures to form a solid superconductor; pressing the solid superconductor at a pressure in a range of from 500 to 1000, 600 to 900, or 700 to 800 MPa into a pre-sintered form; sintering the pre-sintered form at a temperature in a range of from 900 to 1000, 915 to 985, 925 to 975, or 940 to 960° C. for a period in a range of from 4 to 12, 6 to 10, 7 to 9, or 7.5 to 8.5 hours, to obtain a sintered form; and cooling the sintered form at a rate in a range of from 1 to 10, 2 to 7.5, 2.5 to 6, 3 to 5, or 3.5 to 4.5° C./minute to obtain the superconductor. Any of the above permutations of superconductor may be made by such a method.

(17) The atomic ratio or stoichiometry of the YBCO precursor metal oxides may be 1 (Y): 1.9 to 2.1 (Ba): 2.9 to 3.1 (Cu), or 1 (Y): 2 (Ba):3 (Cu). The oxidized form of Y, Ba, and/or Cu, could be a nitrate, a halide, a carbonate, and/or a pure oxide, preferably including Y.sub.2O.sub.3, BaO, BaCO.sub.3, CuO, Cu.sub.2O, CuO.sub.2, and/or Cu.sub.2O.sub.3. The metal oxides may use only three, two, one, or no carbonates, but may preferably use one, or even two, most preferably only BaCO.sub.3, with non-carbonate Y and Cu, preferably Y.sub.2O.sub.3 and CuO.

(18) The WO.sub.3 dopant may present in the range of from 0.01 to 3.0, 0.025 to 2.0, 0.025 to 1.0, 0.05 to 0.5, 0.075 to 0.2 wt. %, based on the total superconductor weight. Because the superconductor may be used for a variety of applications, a desirable doping endpoint may be any of the preceding values as a lower and/or upper end point or at least 0.005, 0.01, 0.02, 0.03, 0.04, 0.05, 0.06, 0.07, or 0.08 wt. %, and/or no more than 0.5, 0.45, 0.4, 0.35, 0.3, 0.25, 0.2, or 0.15

(19) The dopant maybe in a form that includes wire(s), tube(s), sphere(s), prism(s), or a mixture of two or more of any of these nano-structures, preferably at least including nanowires. Preferably at least 99, 99.5, 99.9, 99.98, 99.99 or 100% of the dopant have a nano-wire structure.

(20) Inventive methods may further comprise compressing, such as pelletizing, the oxidized forms of yttrium, barium, and copper into a precursor form prior to the heating. The sintering may be conducted in an atmosphere comprising air, e.g., in at least 50, 60, 75, 85, 90, 95, 97.5, 99, or 100%. The WO.sub.3 nano-structures may comprise 99, 99.5, 99.8, 99.9, 99.99, or 100% nanowires, based on the total number of WO.sub.3 nano-structures, which is also applicable to the superconductors discussed above, and the nanostructure properties discussed above may be applied to the starting material and final, incorporated dopant(s) in inventive methods. The starting material and product dopant(s) will preferably have identical structural properties, ignoring the incorporation of and any particular YBCO-dopant interaction forces.

(21) Inventive superconductors may comprise at least 97, more preferably 98, more preferably 99, more preferably 99.5, more preferably 99.6, more preferably 99.7% YBa.sub.2Cu.sub.3O.sub.7-δ (Y-123), relative to other yttrium-based compounds, wherein, measured volumetrically and/or mass-wise, the Y-123 superconducting material has orthorhombic crystal structure having Pmmm symmetry. The superconductors may contain small amounts, e.g., no more than 1, 0.9, 0.8, 0.7, 0.6, 0.5, 0.4, 0.3% of Y.sub.2BaCuO.sub.5 (Y-211).

(22) Inventive superconductors may have at least 97, more preferably 98, more preferably 99, more preferably 99.5, more preferably 99.6, more preferably 99.7% of Y-123 phase having orthorhombic crystal structure and Pmmm symmetry. The superconductor generally comprises single-phase Y-123. Inventive superconductors may comprise no further phases of YBCO than Y-123, or no more than 3, 2.5, 2, 1, 0.5, 0.4, 0.3%, based on a total weight of any phase beyond Y-123. Inventive superconductors preferably comprise no more than 0.5, 0.25, 0.1, 0.05, 0.01, 0.001 or 0.0001%, or even none to detectable limits, of any further phases of YBCO than Y-123, based on the total material weight. Inventive superconductors may comprise no more than 0.5, 0.25, 0.1, 0.05, 0.01, 0.001 or 0.0001% of Y.sub.2BaCuO.sub.5 (Y-211), and/or YBaCu.sub.2O.sub.5-δ (Y-112), and/or YBa.sub.2Cu.sub.4O.sub.y (Y-124), and/or Y.sub.2Ba.sub.4Cu.sub.7O.sub.y (Y-247), BaCuO.sub.2, based on the total material weight, either individually, or combined. Inventive superconductors, however, under some circumstances, may not desirably contain any of these or further phases.

(23) The superconductors within the scope of the invention preferably do not have additional phases beyond the normal YBCO phase and defined WO.sub.3 dopant, i.e., has no more than 1, 0.9, 0.8, 0.7, 0.6, 0.5, 0.4, 0.3% of Y-211. Preferably, the inventive superconductors maintain nanowires of WO.sub.3 that do not react with YBa.sub.2Cu.sub.3O.sub.7-δ, but instead keep their size and preferably contribute with their volume, interfaces, and/or generated defects that may enhance the critical current density J.sub.cm.

(24) In addition or alternatively, the inventive superconductors are made without chelating ligands on the metals, particularly acetate or acetylacetone (acac). The YBCO used may also be produced from only solids, rather than involving solubilized starting materials, thereby leading to crystal structures as described herein and illustrated in the drawings. The synthesis of superconductors within the invention may be made by any method leading to the claimed structure, but preferably avoids solution phase reactions, particularly avoiding ethylene glycol (glycols generally), ethanol (alcohols generally), and/or water, and can eschew the use of bases, such as ammonia, hydroxides, and the like. Superconductors herein may avoid sustaining temperatures for longer than 1 hour, 45, 30, 15, 10, 5, or 1 minute after the 900+° C. calcining, i.e., an annealing step such as sustained heating in a range of 300 to 600° C. after formation of the YBCO and/or doped YBCO may be avoided.

(25) Inventive superconductors may have in their matrices a regular form of nanometer scale entities bright in contrast dispersed into grains. The nanosized entities may have an average size of 100, 60, 50, 40, 30, or 20 nm in diameter. The nanosized entities are generally well-dispersed, i.e., only 1 in 5, 1 in 10, or 1 in 20 is agglomerated. Inventive superconductors may have in their matrices WO.sub.3 nanowires taking place within the grains boundaries by filling the voids among the grains.

(26) Inventive superconductors may have a superconducting transition in a range of from 80 to 100, 85 to 98, 88 to 97, 91 to 96 K, or at least 85, 87, 89, 90, 91, 92, 93, 94, 95, or even 96 K.

(27) Inventive superconductors may have a critical current density (J.sub.cm) in a range of from 1.0×10.sup.4 to 1.4×10.sup.4, 1.1×10.sup.4 to 1.35×10.sup.4, 1.2×10.sup.4 to 1.3×10.sup.4 A/cm.sup.2, or at least 1, 1.05, 1.1, 1.15, or 1.2×10.sup.4 A/cm.sup.2, in an applied magnetic field of 0 Tesla, and/or a critical current density (J.sub.cm) in a range of from 600 to 800, 650 to 780, or 700 to 750 A/cm.sup.2, or at least 600, 625, 650, 675, or 700 A/cm.sup.2, in an applied magnetic field one of 1 Tesla. Alternatively, or in addition, inventive superconductors may have a critical current density of at least 4×10.sup.3, 10.sup.4, 2×10.sup.4, 3×10.sup.4, 5×10.sup.4, or 10.sup.5 A/cm.sup.2 at temperature range 60, 50, 40, 30, 20, or 10 K, under a magnetic field in a range of from 0 to 6 Tesla. The critical current density of inventive superconductors enhanced in WO.sub.3 added Y-123 compared to non-added Y-123 by factors more than 25, 15, 10, 5, or 2%, at temperature range 77, 70, 60, 50, 40, 30, 20, or 10 K, over the magnetic field range of 0 to 6 Tesla.

Example

(28) Pure YBCO samples and WO.sub.3 nanowire-doped YBCO samples were synthesized through the solid-state reaction method under identical conditions. The single phase YBCO was synthesized by thoroughly mixing high purity of Y.sub.2O.sub.3, BaCO.sub.3, and CuO according to the stoichiometric formula of Y:Ba:Cu=1:2:3. This mixture of powders was pelletized and then calcined at 950° C. for 12 h in air. WO.sub.3 nanowires were added to the precursor powder Y-123 in the final processing stage, by mixing and hand grinding both powders in an agate mortar. The amount of added WO.sub.3 nanowire varied from x=0 to 3 wt. % of the total mass of sample. The mixed powders were pressed into pellets at 750 MPa in the form of circular disks having 13 mm in diameter. The pellets were sintered at 950° C. for 8 hours in air and then cooled to room temperature at a rate of 4° C./min. The non-doped (0 wt. % WO.sub.3) sample was used as a reference, then it was hand ground in the same manner as the WO.sub.3-doped samples to ensure identical physical conditions for all of the samples.

(29) The resulting samples were characterized using x-ray powder diffraction (XRD), scanning electron microscopy (SEM), electrical resistivity versus temperature, and magnetization versus fields M(H) hysteresis loops.

(30) Referring now to the drawings, wherein like reference numerals designate identical or corresponding parts throughout the several views.

(31) FIG. 1 illustrates XRD patterns from all products, indicating that each exhibits a predominantly single-phase perovskite YBa.sub.2Cu.sub.3O.sub.y (Y-123) with a very small quantity of Y.sub.2BaCuO.sub.5 (Y-211) as secondary phase (about 0.3, 0.35, 0.33, 0.35, 0.5, 0.9, 1.6 and 2.2 for 0.0, 0.05, 0.1, 0.2, 0.5, 1.0, 2.0 and 3.0 wt. % WO.sub.3 nanowires added to Y-123 samples, respectively). The synthesized samples crystallized in the orthorhombic structure with Pmmm symmetry. No detrimental effects on the orthorhombicity structure of Y-123 were detected by inserting fine quantities of WO.sub.3 nanowires up to 1 wt. % under the accuracy of XRD patterns. For higher amount of WO.sub.3 nanowires (≥2 wt. %), WO.sub.3 peaks with very low intensity were detected. Therefore, it appears that any phenomenon observed herein for lower amounts (<2 wt. %) of WO.sub.3 nanowire-dopant may be irrelevant to structural change in these YBCO products, but fully associated to the inclusion of WO.sub.3 nanowires.

(32) As seen in FIGS. 2A and B, the morphology of Y-123 doped with WO.sub.3 nanowires exhibits a granular aspect with a dispersion of fine nano-entities that take place on the surface of grains with relatively uniform distribution. In addition, the WO.sub.3 nanowires take place into the grain boundaries by filling the voids among the grains. This could enhance the percolation of current in added sample, particularly the current density J.sub.c.

(33) FIGS. 3A and 3B shows that all Y-123 samples produced according to the Example exhibit a metal-like behavior in the normal state, with a sharp superconducting transition to zero resistance at T.sub.co for lower WO.sub.3 nanowires concentrations, i.e., ≤0.5 wt. %. For higher WO.sub.3 amounts, i.e., >0.5 wt. %, a broadening superconducting transition was observed. The T.sub.co value is found 92.5 K for pristine, undoped compound and the T.sub.co remains unchanged up to 0.5 wt. % doping, then decreases with increasing the WO.sub.3 nanowires contents. Besides, the 0.1 wt. % NW—WO.sub.3 added to Y-123 product exhibit the lowest normal state resistivity compared to pristine sample, suggesting the lowest number of porosity, disorder and inhomogeneity and the highest carrier concentration in this sample. The obtained results suggest the enhancement of flux pinning in this added sample.

(34) FIG. 4 illustrates that the magnetization behavior of the inventive superconductor products described herein and the zero-field value of the magnetization are improved for WO.sub.3 nanowire-doped samples compared to pristine, undoped one Y-123 synthesized according to the Example. For the products synthesized with a low concentration of WO.sub.3 nanowires, e.g., ≤0.1 wt. %, the hysteresis loops M(H) have larger areas and close much later in comparison with those of the pristine product indicating an enhancement of the irreversibility field (H.sub.irr) and current densities values.

(35) The intra-granular critical current density (J.sub.cm) versus magnetic field for various amounts of WO.sub.3 nanowires were estimated from the experiments of M vs. H using Bean's critical-state model are shown in FIG. 5A. Throughout the applied magnetic field range, the 0.1 and 0.2 wt. % WO.sub.3 nanowires added YBCO samples show higher J.sub.cm values compared to the pure Y-123 as synthesized herein. The 0.1 wt. % WO.sub.3-doped sample illustrates better performance and the best J.sub.cm values in the absence and under applied magnetic fields. Furthermore, the 0.1 wt. % WO.sub.3-doped sample exhibits a distinctly higher flux pinning force density, as seen in FIG. 5B. The inclusion of WO.sub.3 nanowires in ranges discussed herein may improve the weak bonds of Y-123, possibly strengthening the flux pinning properties of the doped Y-123 product over the measured magnetic field range. The formation of efficient pinning centers due to dopants and/or additives may affect characteristic behavior(s) of the critical current densities.

(36) As seen in FIG. 7B versus FIG. 7A (undoped), when increasing the WO.sub.3 doping content to 0.1 wt. %, the J.sub.cm value may improve by a factor of 4.3 in the absence of applied magnetic field and at T=77K. Under an external applied magnetic field of 1 Tesla, the J.sub.cm value enhanced by a factor of around 26 (T=77 K). The inclusion of WO.sub.3 nanowires as described herein may assist in achieving high flux pinning performances. FIGS. 7A and 7B show the variations of the intra-granular critical current density J.sub.cm versus field of the free, undoped (FIG. 7A) and 0.1 wt. % WO.sub.3 nanowire-doped samples (FIG. 7B) measured at various temperatures. The results from the Example indicate that the WO.sub.3 nanowires reduce the sensitivity to the magnetic field for a temperature ranging from 10 to 77 K. The rate of the decrease of J.sub.cm with increasing temperature is lower for the WO.sub.3 nanowire-doped sample than for the pristine sample. Across the entire range of the applied magnetic field, the WO.sub.3 nanowire-doped sample exhibits a distinctly higher J.sub.cm in the entire temperature range compared with the pristine one.

(37) FIG. 8 illustrates the temperature dependence of the ratio, R, as set forth in Equation 1, immediately below, at applied magnetic fields of 0 and 1 T.

(38) $\begin{array}{cc}R=\frac{J_{\mathrm{cm}}\left(0.1\mathrm{wt}.\%\mathrm{NW}-{\mathrm{WO}}_3\right)}{J_{\mathrm{cm}}\left(0.\mathrm{wt}.\%\right)},& \mathrm{Eq}.1\end{array}$
wherein J.sub.cm is intra-granular critical current density, NW is the nanowire-doped superconductor, WO.sub.3 is the pure nanowire, and 0.0 wt. % is the pure Y-123. FIG. 8 illustrates that the quotients of J.sub.cm as a function of temperature for the 0.1 wt. % WO.sub.3 nanowires and free added samples for 0 and 1 Tesla applied magnetic fields.

(39) The superconducting materials described herein may be used for application that function to transport higher current densities with very low loss of energy such as in low-loss power and electrical transmission cables; enhance power stability for energy storage such as in fuel cells; improve electromagnetic performance such as in superconducting electromagnets; to generate high magnetic fields for several practical applications. Products, devices and systems may include the superconducting materials for service in transport of higher current densities with very low loss of energy and the generation of high magnetic fields for practical applications.

(40) Numerous modifications and variations of the present invention are possible in light of the above teachings. It is therefore to be understood that within the scope of the appended claims, the invention may be practiced otherwise than as specifically described herein.