Fajardo et al., 2019 - Google Patents
Fabrication of Bi-2212 canted-cosine-theta dipole prototypesFajardo et al., 2019
View PDF- Document ID
- 15104897404108443614
- Author
- Fajardo L
- Brouwer L
- Caspi S
- Hafalia A
- Hernikl C
- Prestemon S
- Shen T
- Bosque E
- English C
- Publication year
- Publication venue
- IEEE Transactions on Applied Superconductivity
External Links
Snippet
The US Magnet Development Program (MDP) is exploring the possibility of combining low- and high-temperature superconductor technologies, using cosine-theta and canted-cosine- theta (CCT) Nb 3 Sn dipole magnets together with Bi-2212 CCT inserts, with the ultimate …
- 238000004519 manufacturing process 0 title abstract description 19
Classifications
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
- H01F6/06—Coils, e.g. winding, insulating, terminating or casing arrangements therefor
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F41/00—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
- H01F41/02—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets
- H01F41/04—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets for manufacturing coils
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H01L39/00—Devices using superconductivity; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof
- H01L39/24—Processes or apparatus peculiar to the manufacture or treatment of devices provided for in H01L39/00 or of parts thereof
- H01L39/2419—Processes or apparatus peculiar to the manufacture or treatment of devices provided for in H01L39/00 or of parts thereof the superconducting material comprising copper oxide
- H01L39/2464—After-treatment, e.g. patterning
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H01L39/00—Devices using superconductivity; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof
- H01L39/24—Processes or apparatus peculiar to the manufacture or treatment of devices provided for in H01L39/00 or of parts thereof
- H01L39/2419—Processes or apparatus peculiar to the manufacture or treatment of devices provided for in H01L39/00 or of parts thereof the superconducting material comprising copper oxide
- H01L39/248—Processes peculiar to the manufacture or treatment of filaments or composite wires
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H01L39/00—Devices using superconductivity; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof
- H01L39/24—Processes or apparatus peculiar to the manufacture or treatment of devices provided for in H01L39/00 or of parts thereof
- H01L39/2419—Processes or apparatus peculiar to the manufacture or treatment of devices provided for in H01L39/00 or of parts thereof the superconducting material comprising copper oxide
- H01L39/2422—Processes for depositing or forming superconductor layers
- H01L39/2454—Processes for depositing or forming superconductor layers characterised by the substrate
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01B—CABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
- H01B12/00—Superconductive or hyperconductive conductors, cables, or transmission lines
- H01B12/16—Superconductive or hyperconductive conductors, cables, or transmission lines characterised by cooling
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H01L39/00—Devices using superconductivity; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof
- H01L39/02—Details
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/0036—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties showing low dimensional magnetism, i.e. spin rearrangements due to a restriction of dimensions, e.g. showing giant magnetoresistivity
- H01F1/0072—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties showing low dimensional magnetism, i.e. spin rearrangements due to a restriction of dimensions, e.g. showing giant magnetoresistivity one dimensional, i.e. linear or dendritic nanostructures
- H01F1/0081—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties showing low dimensional magnetism, i.e. spin rearrangements due to a restriction of dimensions, e.g. showing giant magnetoresistivity one dimensional, i.e. linear or dendritic nanostructures in a non-magnetic matrix, e.g. Fe-nanowires in a nanoporous membrane
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01B—CABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
- H01B3/00—Insulators or insulating bodies characterised by the insulating materials; Selection of materials for their insulating or dielectric properties
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01B—CABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
- H01B7/00—Insulated conductors or cables characterised by their form
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GASES [GHG] EMISSION, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/60—Superconducting electric elements or equipment or power systems integrating superconducting elements or equipment
- Y02E40/64—Superconducting transmission lines or power lines or cables or installations thereof
- Y02E40/641—Superconducting transmission lines or power lines or cables or installations thereof characterised by their form
- Y02E40/642—Films or wires on bases or cores
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GASES [GHG] EMISSION, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/60—Superconducting electric elements or equipment or power systems integrating superconducting elements or equipment
- Y02E40/64—Superconducting transmission lines or power lines or cables or installations thereof
- Y02E40/641—Superconducting transmission lines or power lines or cables or installations thereof characterised by their form
- Y02E40/644—Multifilaments embedded in normal conductors
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Fajardo et al. | Fabrication of Bi-2212 canted-cosine-theta dipole prototypes | |
| Van der Laan et al. | Status of CORC® cables and wires for use in high-field magnets and power systems a decade after their introduction | |
| Wolf et al. | HTS CroCo: A stacked HTS conductor optimized for high currents and long-length production | |
| Takayasu et al. | Conductor characterization of YBCO twisted stacked-tape cables | |
| Zhang et al. | Progress in production and performance of second generation (2G) HTS wire for practical applications | |
| Mulder et al. | Design and manufacturing of a 45 kA at 10 T REBCO-CORC cable-in-conduit conductor for large-scale magnets | |
| Wang et al. | Development of a quasi-isotropic strand stacked by 2G wires | |
| Godeke et al. | Wind-and-react Bi-2212 coil development for accelerator magnets | |
| Mulder et al. | Development of ReBCO-CORC wires with current densities of 400–600 A/mm $^ 2$ at 10 T and 4.2 K | |
| Arbelaez et al. | Status of the Nb $ _ {3} $ Sn canted-cosine-theta dipole magnet program at Lawrence Berkeley National Laboratory | |
| Takayasu et al. | Investigation of twisted stacked-tape cable conductor | |
| US5187859A (en) | Method of preloading superconducting coils by using materials with different thermal expansion coefficients | |
| Godeke et al. | Bi-2212 canted-cosine-theta coils for high-field accelerator magnets | |
| Yanagi et al. | Progress of the design of HTS magnet option and R&D activities for the helical fusion reactor | |
| Garcia Fajardo et al. | First demonstration of high current canted-cosine-theta coils with Bi-2212 Rutherford cables | |
| Shen et al. | Design, fabrication, and characterization of a high-field high-temperature superconducting Bi-2212 accelerator dipole magnet | |
| Wolf et al. | Critical current densities of 482 A/mm 2 in HTS crossconductors at 4.2 K and 12 T | |
| Yang et al. | In situ detection of delamination and critical current degradation caused by the thermal stress in epoxy impregnated REBa2Cu3O7− δ coils | |
| Shi et al. | Quasi-round HTS conductor using REBCO tapes for fusion magnet application | |
| Sumption et al. | AC losses of Roebel and CORC® cables at higher AC magnetic fields and ramp rates | |
| Kováč et al. | Tensile and bending strain tolerance of ex situ MgB 2/Ni/Cu superconductor tape | |
| Marken et al. | Progress in $ rm Bi $-2212 Wires for High Magnetic Field Applications | |
| van der Laan et al. | CORC® wires allowing bending to 20 mm radius with 97.5% retention in critical current and having an engineering current density of 530 A mm− 2 at 20 T | |
| Castaneda et al. | A 6-around-1 cable using high-temperature superconducting STAR® wires for magnet applications | |
| Godeke et al. | Progress in wind-and-react Bi-2212 accelerator magnet technology |