By E. W. Collings (auth.)
Scope and goal even supposing conductors in keeping 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 serious present densities to degrade quickly lower than rigidity, have commonly limited their use to rather trouble-free, frequently 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 top severe box, has no longer three entered common carrier. pressure has been chanced on to don't have any measurable impact on both the severe fields or the serious present densities of compound superconductors with BI and Cl5 crystal constructions, yet as but they're nonetheless within the examine and improvement phases. nonetheless, conductors utilizing the binary alloy Ti-Nb or multi part alloys according to it, due to their relative ease of manufacture, first-class mechanical houses, and comparatively low pressure sensitivities, at the moment are being pressed into provider 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 cord for superconducting The use magnet purposes used to be first proposed in 1961. through the resulting ten years, whereas development used to be 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 platforms within the primary learn of type-II superconductivity.
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Additional resources for Applied Superconductivity, Metallurgy, and Physics of Titanium Alloys: Fundamentals Alloy Superconductors: Their Metallurgical, Physical, and Magnetic-Mixed-State Properties
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. 2 Tc in the w + /3-Phase Alloys . . . 1 Typical Results . . . . . 2 Atypical Results-Ti-Mn ....
9 Conclusion-Summary of Essential Factors Controlling the Magnitude of the Upper Critical Field . . . . . Chapter 16. 1 Introduction . . . . . . . . 3 The Elementary Pinning Force, /p . . . 3 Critical State Models . . . . . . 4 The Bean Model of the Critical State . . . 5 Models for the Pinned Critical State ....... 6 Applications of the Critical State Models to Tube and Coil 566 567 568 569 570 571 571 573 578 Magnetization . . . . . . . . 1 Tube and Coil Magnetization Studies-A General Introduction .
499 500 500 502 502 504 506 506 506 507 507 507 510 513 514 514 517 517 518 518 518 518 518 519 519 519 520 520 520 520 521 Contents xl Chapter 15. 1 Pauli Paramagnetic Limitation . . . . . . . 1 Early Observations . . . . . . . 2 Thermodynamic Model for the SOS Relief of PPL . 3 Mechanistic Interpretation of the SOS/PPL Effects. 4 The Spin-Paramagnetic Theories of Maki and of Werthamer, Helfand, and Hohenberg . . . . . . . . 1 The Theories of Maki . . . . . . . .
Applied Superconductivity, Metallurgy, and Physics of Titanium Alloys: Fundamentals Alloy Superconductors: Their Metallurgical, Physical, and Magnetic-Mixed-State Properties by E. W. Collings (auth.)