By E. W. Collings (auth.)

Scope and function even if conductors in accordance with the Al5 intermetallic compound Nb Sn three own fascinating high-field superconducting homes, production and dealing with problems, coupled with the tendency in their severe present densities to degrade speedily below pressure, have as a rule constrained their use to particularly basic, often small-scale solenoidal-magnet applica­ tions. Likewise the Al5 compound VGa, which has a much wider severe pressure three window than NbSn yet a uniformly decrease higher serious box, has now not three entered common provider. pressure has been came across to haven't any measurable impact on both the serious fields or the serious present densities of compound superconductors with BI and Cl5 crystal constructions, yet as but they're nonetheless within the study and improvement levels. nonetheless, conductors utilizing the binary alloy Ti-Nb or multi part alloys in keeping with it, due to their relative ease of manufacture, very good mechanical houses, and comparatively low pressure sensitivities, at the moment are being pressed into carrier in different large-scale units. Such conductors are being wound into magnets to be used in power garage, strength conversion (i. e. , turbines and motors), and high-energy particle detectors and beam-handling magnets. of cold-rolled or drawn Ti-Nb-alloy twine for superconducting The use magnet functions was once first proposed in 1961. through the resulting ten years, whereas growth was once being made within the improvement of Cu-clad filamentary-Ti-Nb-alloy conductors, Ti-Nb and different Ti-base binary transi­ tion-metal (TM) alloys have been being hired as version structures within the basic examine of type-II superconductivity.

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Extra info for Applied Superconductivity, Metallurgy, and Physics of Titanium Alloys: Fundamentals Alloy Superconductors: Their Metallurgical, Physical, and Magnetic-Mixed-State Properties

Sample text

A) Modified Weak-Coupling Approach (b) Strong-Coupling Approach . . (c) Prognosis for Ti-Nb . . . . 1 Parallel Strips . . . . 3 Granular Compacts ..... 4 Fiber-Reinforced Composites (a) The Longitudinal Thermal Expansion (b) Transverse Thermal Expansion (c) Thermal Expansion Data for Some Superconducting Magnet Composites . . . . . . . 356 357 358 358 360 361 361 361 361 363 363 363 366 367 367 369 370 370 372 373 373 375 375 376 377 377 377 379 379 III: THE SUPERCONDUCTING TRANSITION Chapter 10.

1 General Description . . . . . . . . 2 Low-Temperature Specific Heats of Ti-V, Ti-Mo, and TiFe . . . . . . . . . . . . 1 Experimental Observations . . . . . . . 2 Lattice Specific Heat in the Normal and Superconducting States ................. 4 The Superconductive Electronic Specific Heat . 2 The Exponential Form . . . . . 4 The Electronic Specific Heat at Te~Height of the Specific Heat Jump, IlC . . . . . . . . 5 The Electron-Phonon Coupling Strength .

1 Symbols for the Upper Critical Fields . . . 5 Final Developments in Nonparamagnetic Mixed-State Theory ..................... 6 Evaluation of the Nonparamagnetic Upper Critical Field.. e-State Properties . . . 2 A Case Study with Ti-Nb . . . 1 HelO in Terms of Measurable Parameters (a) The Method of Fietz and Webb for Irreversible Superconductors . . . . . . . . (b) The Method of Lubell and Kernohan . . . 2 Validity of Nonparamagentic Maki Theory as a Descriptor of Hel in Intermediate-KGL Alloys-A Case Study of TiDoped Nb .

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