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critical current density
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in High-Temperature Superconductors for Wires and Tapes[1]
> Properties and Selection: Nonferrous Alloys and Special-Purpose Materials
Published: 01 January 1990
Fig. 1 Plot of critical current density versus magnetic flux density to compare properties of powder-in-tube process oxide-base superconductors with that of conventional superconductors. MRI, magnetic resonance imaging; SSC, superconducting supercollider
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in Principles of Superconductivity
> Properties and Selection: Nonferrous Alloys and Special-Purpose Materials
Published: 01 January 1990
Fig. 8 Scaling law behavior of the critical current density ( J c ) for (a) several niobium-titanium alloys ( Ref 25 ) and (b) a Nb 3 Sn conductor ( Ref 26 ). In both cases, F p = J c B is plotted, scaled by the maximum value versus the reduced applied magnetic field, h = H a / H
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in Niobium-Titanium Superconductors
> Properties and Selection: Nonferrous Alloys and Special-Purpose Materials
Published: 01 January 1990
Fig. 28 Plot of critical current density versus strain (since the last precipitation heat treatment) for a multifilamentary composite that received 4, 5, 6, 7, and 8 heat treatments. Courtesy of Supercon, Inc.
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in Ternary Molybdenum Chalcogenides (Chevrel Phases)
> Properties and Selection: Nonferrous Alloys and Special-Purpose Materials
Published: 01 January 1990
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in High-Temperature Superconductors for Wires and Tapes[1]
> Properties and Selection: Nonferrous Alloys and Special-Purpose Materials
Published: 01 January 1990
Fig. 3 Plot of critical current density versus external magnetic field at 4.2 K to compare two silver-sheathed powder-in-tube superconducting oxide wires (Bi-2212/Ag and YBa 2 Cu 3 O 7 ) with three conventional multifilamentary wires. J c data is for superconductor cross section, also
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in High-Temperature Superconductors for Wires and Tapes[1]
> Properties and Selection: Nonferrous Alloys and Special-Purpose Materials
Published: 01 January 1990
Fig. 5 Plot of critical current density versus external magnetic field at measurement temperature of 77 K to compare sintered powder YBCO tape-shaped wire with melt-processed YBCO tape-shaped wire. Source: Ref 21
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in Electrical/Electronic Applications for Advanced Ceramics
> Engineered Materials Handbook Desk Edition
Published: 01 November 1995
Fig. 45 Critical current density of a polycrystalline ceramic specimen compared with a silver substrate as a function of applied magnetic field
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Published: 01 January 1990
Fig. 13 Grain size dependence of critical current densities for bronze-processed Nb 3 Ga, V 3 Ga, and V 3 Si at 4.2 K and H = 4 T (40 kG). Source: Ref 13
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Published: 01 December 1998
Fig. 1 Critical temperature, current density, and magnetic field boundary separating superconducting and normal conducting states. These data, which are for a niobium-titanium superconducting alloy, are based on measurements at 4.2 K.
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Series: ASM Handbook
Volume: 2
Publisher: ASM International
Published: 01 January 1990
DOI: 10.31399/asm.hb.v02.a0001111
EISBN: 978-1-62708-162-7
... Abstract This article reviews the phase diagrams, alloy with third element additions, layer growth, critical current density, and matrix materials of A15 superconductors. It describes the production methods of tape conductors (chloride deposition, and surface diffusion) and multifilamentary...
Abstract
This article reviews the phase diagrams, alloy with third element additions, layer growth, critical current density, and matrix materials of A15 superconductors. It describes the production methods of tape conductors (chloride deposition, and surface diffusion) and multifilamentary wires (rod process, modified jelly roll process, niobium tube process, in-situ process, powder metallurgy process, and jelly roll method). The article focuses on reaction heat treatment, which is required at the end of wire processing to convert the ductile components to the desired, but brittle, superconductor. Finally, it discusses the applications of A15 superconductors in commercial magnets, power generation, power transmission, high-energy physics, and fusion.
Series: ASM Handbook
Volume: 2
Publisher: ASM International
Published: 01 January 1990
DOI: 10.31399/asm.hb.v02.a0001114
EISBN: 978-1-62708-162-7
... for microcracking. These processing problems, however, are balanced to some degree by the ability to produce a high percentage of single-phase material if the processing is properly followed. A fairly high 92 K superconducting transition and production of satisfactory critical current density in idealized thin-film...
Abstract
The discovery of the high-critical-temperature oxide superconductors has accelerated the interest for superconducting applications due to its higher-temperature operation at liquid nitrogen or above and thus reduces the refrigeration and liquid helium requirement. It also permits usage of the high-critical-temperature oxides in magnets or power applications in high-current-carrying wire or tape with acceptable mechanical capability. This article discusses the powder techniques mainly based on the production of an oxide powder precursor, which is then subjected to various processing, including powder-in-tube processing, vapor deposition processing, and melt processing. It further discusses the microstructural, anisotropy and weak link influences on these processes.
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Published: 01 January 2003
Series: ASM Handbook
Volume: 2
Publisher: ASM International
Published: 01 January 1990
DOI: 10.31399/asm.hb.v02.a0001109
EISBN: 978-1-62708-162-7
... Critical temperature, T c at 0 T Parameters at 4.2 K Thermodynamic critical field, T, at Magnetic penetration depth (λ), nm Coherence length (ξ) nm Critical current density ( J c ), kA · mm −2 μ 0 H c μ 0 H c1 μ 0 H c2 Pb I 7.3 0.0803 (a) … … 40 83 … Nb II 9.3...
Abstract
Superconductivity has been found in a wide range of materials, including pure metals, alloys, compounds, oxides, and organic materials. Providing information on the basic principles, this article discusses the theoretical background, types of superconductors, and critical parameters of superconductivity. It discusses the magnetic properties of selected superconductors and types of stabilization, including cryogenic stability, adiabatic stability, and dynamic stability. The article also focuses on alternating current losses in superconductors, including hysteresis loss, penetration loss, eddy current loss, and radio frequency loss. Furthermore, the article describes the flux pinning phenomenon and Josephson effects.
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in Principles of Superconductivity
> Properties and Selection: Nonferrous Alloys and Special-Purpose Materials
Published: 01 January 1990
Fig. 19 The critical state model of flux penetration into a superconducting slab. As the applied field is raised from zero (a and b), the field penetrates the surface of the superconductor to a depth p The gradient of the field (∂ B /∂ x is equal to the critical current density ( J c
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Series: ASM Handbook
Volume: 2
Publisher: ASM International
Published: 01 January 1990
DOI: 10.31399/asm.hb.v02.a0001112
EISBN: 978-1-62708-162-7
... knowledge of this reaction, the primary effect is certainly to change the stoichiometry of the central powder and hence its properties. Nevertheless, no one has given up on this process, for this drawback is counterbalanced by both the ease of the cold drawing technique and the critical current densities...
Abstract
Ternary molybdenum chalcogenides stands for a vast class of materials, whose general formula is MxMO6X8, where, M is a cation and X is a chalcogen (sulfur, selenium, or tellurium). Possible applications of some of these are as high field superconductors (that is, >20 T, or 200 kG). This article discusses the fabrication methods of PbMo6S8 (PMS) and SnMo6S8 (SMS), including hot processing and cold processing. It provides a short note on the superconducting properties of PMS wire filaments and their applications in processes requiring high magnetic fields, such as high-energy physics, thermonuclear fusion, and nuclear magnetic resonance.
Series: ASM Handbook
Volume: 2
Publisher: ASM International
Published: 01 January 1990
DOI: 10.31399/asm.hb.v02.a0001113
EISBN: 978-1-62708-162-7
.... They each exhibit planes of Cu-O in the a-b plane, which seems critical to the superconductivity of the materials. As a result, they are all highly anisotropic with a substantial drop in superconducting properties (for example, critical current density, J c ), when the c -axis is parallel rather than...
Abstract
This article focuses on different thin-film deposition techniques used to make superconducting films and discusses the properties and advantages of high-critical-temperature and low-critical-temperature materials in a number of applications, including signal processing and analog electronic devices. The article gives a brief introduction on superconducting materials, substrates and buffer layers and discusses the major deposition techniques such as, electron-beam co-evaporation, sputtering from either a composite target or multiple sources and laser ablation. The article also describes the in-situ film growth techniques for producing atomic oxygen by radio frequency excitation or microwave discharge or with ozone.
Book Chapter
Series: ASM Desk Editions
Publisher: ASM International
Published: 01 December 1998
DOI: 10.31399/asm.hb.mhde2.a0003155
EISBN: 978-1-62708-199-3
... 100 K. At temperatures below T c , the superconducting state will cease upon application of a sufficiently large magnetic field, termed the critical field, H c , which depends on temperature and decreases with increasing temperature. The same is true for current density; that is, a critical...
Abstract
Superconductors are materials that exhibit a complete disappearance of electrical resistivity on lowering the temperature below the critical temperature. A superconducting material must exhibit perfect diamagnetism, that is, the complete exclusion of an applied magnetic field from the bulk of the superconductor. Superconducting materials that have received the most attention are niobium-titanium superconductors (the most widely used superconductor), A15 compounds (in which class the important ordered intermetallic Nb3Sn lies), ternary molybdenum chalcogenides (Chevrel phases), and high-temperature ceramic superconductors. This article provides an overview of basic principles of superconductors and the different classes of superconducting materials and their general characteristics.
Series: ASM Handbook
Volume: 2
Publisher: ASM International
Published: 01 January 1990
DOI: 10.31399/asm.hb.v02.a0001110
EISBN: 978-1-62708-162-7
..., there is little the wire manufacturer can do to alter them. It is the critical current density ( J c ) that is most affected by the processing from cast ingot to final wire and cable. The superconducting properties, therefore, are highly dependent on the cooling rate following melting or heat treatment...
Abstract
Niobium-titanium alloys (NbTi) became the superconductors of choice in the early 1960s, providing a viable alternative to the A-15 compounds and less ductile alloys of niobium-zirconium. This can be attributed to the relative ease of fabrication, better electrical properties, and greater compatibility with copper stabilizing materials. This article discusses the ramifications of design requirements, selection criteria and processing methods of superconducting fibers and matrix materials. It provides information on the various steps involved in the fabrication of superconducting composites, including assembly, welding, isostatic compaction, extrusion, wire drawing, twisting, and final sizing. The article also provides a detailed account of the properties and applications of NbTi superconducting composites.
Book Chapter
Series: ASM Handbook
Volume: 2
Publisher: ASM International
Published: 01 January 1990
DOI: 10.31399/asm.hb.v02.a0005549
EISBN: 978-1-62708-162-7
... by experimental reactor ECM electrochemical machining ITS International Temperature Scale EPC evaporative pattern casting the magnet J joule EDM electrical discharge machining HAZ heat-affected zone Je critical current density EEC European Economic Community HB Brinell hardness; horizontal k karat ELI extra-low...
Series: ASM Handbook
Volume: 13A
Publisher: ASM International
Published: 01 January 2003
DOI: 10.31399/asm.hb.v13a.a0003585
EISBN: 978-1-62708-182-5
... current density i p . The critical current density for passivation is i c . Another more practical definition has been provided by an ASTM standard: “passive—the state of metal surface characterized by low corrosion rates in a potential region that is strongly oxidizing for the metal” ( Ref 9...
Abstract
This article reviews the types of passivity and presents tactics that employ passivity to control corrosion. Thermodynamics provides a guide to the conditions under which passivation becomes possible. A valuable guide to thermodynamics is the potential-pH diagram and the Pourbaix diagram. The article presents a potential-pH diagram for the iron-water system and an illustration of an idealized anodic polarization curve for a metal surface, which serves as a basis for describing the kinetics of passivation. It discusses five properties of passive films: thickness, composition, structure, electronic properties, and mechanical properties. The article outlines three possible processes that can form passive films: direct film formation, dissolution precipitation, and anodic oxidation of metal ions in solution. It describes the breakdown of the passive film using various models and highlighting the effect of alloy composition and structure.
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