1999
DOI: 10.1109/77.784666
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Low field flux jumping in high performance multifilamentary Nb/sub 3/Al and Nb/sub 3/Sn composite strands

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Cited by 11 publications
(5 citation statements)
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“…The first column shows the amplitude of the hysteresis loop ΔM at 3 T and 1.9 K for each sample; this value was chosen as parameter to quantify the magnetization of the sample in the field region where flux jumps do not take place. The next columns present the 4 and 5, one can notice that the maximum flux jump amplitude at 1.9 K is correlated to the magnetization of the sample: the larger the magnetization the larger the flux jump amplitude. This relationship is particularly clear when plotting the magnetization of each sample just before it experiences the largest flux jump and the amplitude of this flux jump (Fig.…”
Section: A Flux Jumps Analysismentioning
confidence: 98%
See 1 more Smart Citation
“…The first column shows the amplitude of the hysteresis loop ΔM at 3 T and 1.9 K for each sample; this value was chosen as parameter to quantify the magnetization of the sample in the field region where flux jumps do not take place. The next columns present the 4 and 5, one can notice that the maximum flux jump amplitude at 1.9 K is correlated to the magnetization of the sample: the larger the magnetization the larger the flux jump amplitude. This relationship is particularly clear when plotting the magnetization of each sample just before it experiences the largest flux jump and the amplitude of this flux jump (Fig.…”
Section: A Flux Jumps Analysismentioning
confidence: 98%
“…The high J c, which is more than two times larger than the one of ITER type wires, is obtained at the expense of a large effective filament size D eff of the superconductor. In these wires each sub-element acts as a single filament: in Powder In Tube (PIT) wires the sub-element is constituted of a Nb tube filled with Nb-Sn powder, and during the reaction the tin diffuses transforming the Nb tube into a Nb 3 and the large D eff cause a huge magnetization within the conductor that might compromise the magnet field quality [4]- [8]. Indeed such a large magnetization not only implies a specific design of the magnets to compensate for the field contribution of the persistent currents, but also generates fluxjumps [4]- [8].…”
Section: Introductionmentioning
confidence: 99%
“…5,6 Moreover, there are still open questions related to flux jumping in general, namely, that samples often appear more stable experimentally than predicted by theories. 1 In investigations of such avalanche events, one can benefit significantly by using thin-film samples, where one can visualize the development of the instability by monitoring spatial distributions of the magnetic flux.…”
Section: -3mentioning
confidence: 99%
“…Large flux jumps can even cause magnet quenching. The flux jump behavior of Nb 3 Sn strands in the absence of transport current has been intensively studied [8][9][10][11][12]. Early works by Swartz [8] and Wilson [9] led to criteria for magnetization flux jumps in the adiabatic limit.…”
Section: Introductionmentioning
confidence: 99%
“…Early works by Swartz [8] and Wilson [9] led to criteria for magnetization flux jumps in the adiabatic limit. Sumption et al [10][11][12] early on measured the properties and described the characteristics of the low-field flux jump regime of the new high performance, large d eff Nb 3 Sn conductors for high energy physics applications.…”
Section: Introductionmentioning
confidence: 99%