2002
DOI: 10.1016/s0011-2275(02)00038-3
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The unified strain and temperature scaling law for the pinning force density of bronze-route Nb3Sn wires in high magnetic fields

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Cited by 34 publications
(60 citation statements)
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“…4͑b͔͒. This behavior has been also observed by other groups in MgB 2 , 13,15 Nb 3 Sn, 26,27 and NbTi ͑Ref. 5͒ and, therefore, may not be considered as material specific, but caused by a distribution of parameters determin- ing F p combined with the particular choice of B * .…”
Section: Flux Pinning Curvessupporting
confidence: 58%
“…4͑b͔͒. This behavior has been also observed by other groups in MgB 2 , 13,15 Nb 3 Sn, 26,27 and NbTi ͑Ref. 5͒ and, therefore, may not be considered as material specific, but caused by a distribution of parameters determin- ing F p combined with the particular choice of B * .…”
Section: Flux Pinning Curvessupporting
confidence: 58%
“…The new apparatus allows us to measure the strand in compression and tension to cover a range of applied strain typically from −1 % to +1 %, based on Cheggour's original design [18,19] ("Durham probe" using a "Walter's spring" technique [20]). The variable temperature design utilizes our high-rate helium gas flow and gas temperature pre-regulation approach that was developed at NIST.…”
Section: New Variable Strain/temperature/magnetic-field Apparatusmentioning
confidence: 99%
“…20,34 A third characteristic of wires is the presence of residual strain. Macroscopically, the strain dependence on 0 H K ͑T͒ is well understood in terms of axial strain, [35][36][37] or deviatoric strain, 38,39 but its influence on the complete H-T phase transition is still uncertain. 40 The large Cu matrix enforces a compressive axial strain on the A15 layers due to the larger contraction of the Cu with respect to the A15.…”
Section: Introductionmentioning
confidence: 99%
“…2 Expressions for the H-T phase transition, derived directly from the BCS theory, are readily available in the literature, [44][45][46][47][48][49][50][51][52] and have been applied with success to welldefined laboratory specimens, 1,17,53,54 but most of the H-T data on wires are empirically described. 36,37,41 This leads to continuing discussions in the literature, partly resulting from the use of extrapolated values of 0 H c2 ͑0͒ without taking into account the inhomogeneous nature of the conductors. Although such empirical relations in principle yield sufficient accuracy for the scaling of J c , 42 large discrepancies occur between the fitted values for 0 H K ͑0͒ and T c ͑0͒ and actual measurements.…”
Section: Introductionmentioning
confidence: 99%