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. Author manuscript; available in PMC: 2024 Oct 23.
Published in final edited form as: Supercond Sci Technol. 2017;30(3):10.1088/1361-6668/30/3/033005. doi: 10.1088/1361-6668/30/3/033005

Table 4.

ESE parameter values for combining minimum datasets for Ic(B,T) and Ic(ε) from two different measurement apparatuses. These were obtained with equation-set (11) and the Exponential model for bc2(ε). Two fitting procedures were used: a simultaneous fit for well-matched datasets (top part of the table) and a three-step iterative procedure for mismatched datasets (lower part). Red italic type indicates the parameters that can be determined by each limited dataset (as listed in table 3). By iterating, these values are then used to fix parameter values in the next step (indicated in bold type). Data are for a Nb3Sn conductor made by Luvata, billet #NT8404 ITER-TF conductor, trimmed at FP<100 AT, T>12K. Source data for both datasets are given as Excel files online in the supplemental website.

Core scaling parameters
Parameters: C Bc2(0,0) (T) Tc(0) (K) η s εl0 (%) C1 p q
Simultaneous fit, Ic criterion = 0.1 μV cm−1 for both datasets
14 955 29.74 16.43 1.966 1.4 −0.321 0.657 0.562 1.703
Three-step iterative fit (temp-strain-temp), strain data Ic crit = 1 μV cm−1, temp data Ic crit = 0.1 μV cm−1
1 Ic(B,T) 0.1μV cm−1 14 087 28.49 16.19 1.966 1.4 bc2(ε) 0.562 1.710
2 Ic(ε) 1μV cm−1 18 050 28.49 16.19 1.966 1.4 −0.318 0.616 0.562 1.710
3 Ic(B,T) 0.1μV cm−1 14 930 29.70 16.41 1.966 1.4 −0.318 0.616 0.562 1.710