2019
DOI: 10.1109/tasc.2019.2895197
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High-Performance Bi-2212 Round Wires Made With Recent Powders

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Cited by 67 publications
(75 citation statements)
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“…The feasible quench detection and possible quench-free operation for standalone Bi-2212 magnets enables magnet use of the unique characteristics so far only found in Bi-2212, a combination of high stability that comes with high-T c cuprate superconductors, isotropic behavior due to the round, multifilamentary wire architecture, and the ability to produce long wires and cables with high uniformity and current sharing. With these capabilities, Bi-2212 has taken a huge step towards practical applications such as user-friendly, [25][26][27][28][29][30] T class solenoid research magnets 42 , 20-T class, canted cosine theta geometry 43,44 , accelerator magnets useful for future high-energy colliders, including a high-energy LHC upgrade, and >1.3 GHz NMR magnets due to Bi-2212 being the only isotropic, multifilamentary HTS round wire that permits high magnetic field quality. holding steps during which coil inductive signals die away and noise is much reduced b.…”
Section: Discussionmentioning
confidence: 99%
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“…The feasible quench detection and possible quench-free operation for standalone Bi-2212 magnets enables magnet use of the unique characteristics so far only found in Bi-2212, a combination of high stability that comes with high-T c cuprate superconductors, isotropic behavior due to the round, multifilamentary wire architecture, and the ability to produce long wires and cables with high uniformity and current sharing. With these capabilities, Bi-2212 has taken a huge step towards practical applications such as user-friendly, [25][26][27][28][29][30] T class solenoid research magnets 42 , 20-T class, canted cosine theta geometry 43,44 , accelerator magnets useful for future high-energy colliders, including a high-energy LHC upgrade, and >1.3 GHz NMR magnets due to Bi-2212 being the only isotropic, multifilamentary HTS round wire that permits high magnetic field quality. holding steps during which coil inductive signals die away and noise is much reduced b.…”
Section: Discussionmentioning
confidence: 99%
“…The 4.2 K wire current density J E of the optimally processed strand used in this study is shown in Figure 1 28 . J E is greater than that of the HL-LHC RRP (Rod Restack Process) Nb 3 Sn strand above 11 T and it also has a much less field-sensitive characteristic, achieving 1365 A/mm 2 at 15 T, twice the target desired by the Future Circular Collider (FCC) for Nb 3 Sn strands 31 , and 1000 A/mm 2 at 27 T, 65% better than the previous record Bi-2212 performance 32 .…”
Section: The High Critical Current Density Of These Bi-2212 Wiresmentioning
confidence: 99%
“…For Nb 3 Sn, the conductor properties for the High Luminosity LHC low-β quadrupole magnet is used [27]. The latest record performance for Bi-2212 round wire is from [28]. Three cable candidates are considered for REBCO, the Roebel cable [29], the CORC R wire [30] and the symmetric tape round (STAR) wire [31].…”
Section: Introductionmentioning
confidence: 99%
“…Other cable configurations such as twisted-stack [32] and exfoliated REBCO cable [33] may also be viable for accelerator magnet applications. [35] 26 [8] 105 [8] 110 [36] Upper critical field at 20 K T 0 0 9 [8] 100 [36] Typical wire diameter mm 1.065 [24] 0.85 [27] 0.80 [28] 12×1.5 [37] 3.7 [38] 1.3 [34] J e at 16 T, 4.2 K a A mm −2 0 474 [39] 1300 [28] 964 b [40] 310 c [38] 695 d [34] J e at 20 T, 4.2 K A mm −2 0 123 [39] 1180 [28] 821 b [40] 267 c [38] [43] 30 [38] 15 [34] Effective filament diameter f µm 7 [24] 55 [27] 130 [44] 2-5500 g [22] 2000 g [38] 1400-2500 g [34] Magnetization at 4.2 K, 1 T h mT 10 i [45] 270 [46] 60 [47] 716 j [48] 502 [49] TBD Strand transposition -Full Full Partial Peak heat treatment temperature…”
Section: Introductionmentioning
confidence: 99%
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