By E.W. Collings
In under twenty years the concept that of supercon In each box of technological know-how there are one or ductivity has been reworked from a laboratory participants whose commitment, mixed with an innate interest to usable large-scale functions. within the knowing, lets them have the capacity to snatch, past due 1960's the idea that of filamentary stabilization condense, and clarify to the remainder of us what that published the usefulness of 0 resistance into the sector is all approximately. For the sphere of titanium alloy market, and the commercial forces that force tech superconductivity, such someone is Ted Collings. nology quickly all in favour of niobium-titanium alloys. They His historical past as a metallurgist has probably given him are ductile and hence fabricable into functional tremendous a special virtue in figuring out superconduc undertaking wires that experience the serious currents and tivity in titanium alloys as the optimization of fields useful for large-scale units. greater than superconducting parameters in those alloys has been ninety% of all present-day functions of superconductors nearly completely metallurgical. merits in use titanium alloys. The force to optimize those education and innate skills though, it's alloys led to a flood of study that has been the author's commitment that's the crucial com accrued, condensed, and analyzed during this volume.
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Additional resources for A Sourcebook of Titanium Alloy Superconductivity
E. the transformer. 4 at H e; 1953. Results of a critical review of the literature through (dH/clT)T=T Vickers hardness: Wire prepared by cold swaging crystal bar Ti. (dH/d\)T=T = 400 De K- 1 Vickers hardness: '70 kg mm- 2 . bar") origin unknown. 6;; 20 De -f Purity: c Literature T. S. Smith et at. 387 Trans; tion Temperature. Mutual inductance at 96 Hz. 5" e annealed, 67 kg mm- 2 • as-received, 76 kg mm- 2 ; Iodide process Ti (commonly referred to as "crystal (dH/dTlT=T Vickers hardness: Iodide process Ti obtained from the Foote Mineral Co.
Anomalous scattering mechanisms i ng of superconduct i ve f1 uctuati ons. e. Hake ( 1970) Kohler's-law behaviOUr was excluded on temperature-dependence grounds -- the increase the context of Ti -Fe alloys. Hake [Vet68] ( 1968) J. B. 244] E. M. Sav; tski i made at temperatures between 10 and 20 K Electrical )'esistivity measurements were Ti -Mo. %). 500 and 600"C. 1 in. thickness. Triple arc-melted buttons sectioned The Nb-33Zr of the day was capable of about 2xl0 5 A cm- 2 in that field [Hak6Z a ].
98%). 8',6K low temperature specific heat. (w-phase). A Tc,r', was obtained by extrapolating the single-phase G segment of the curve of Te va Mo concentration. of \ curve, and consequently is more nearly representative But the "13-Ti value" obtained was the result of \. 8%, Johnson and The Te lJl'! composition curve was one of the earl iest true representations of the influence of quenched value for Tc (s-Ti) was fortuitous. annealed (60h/700°C plus 30 h step-cooled to room temperature) samples.