2019
DOI: 10.1109/tasc.2019.2897868
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Inductance of Low-Frequency Small-Scale High-Temperature Superconducting Coils

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Cited by 15 publications
(7 citation statements)
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“…At the very beginning, the inductance value of the HTS coil is about 90% of the normal one (108 mH for HTS coil and 118.9 mH for normal coil) and gradually increasing with the transport current, in agreement with previous findings [41]. Later, when the transport current reaches 11 A, the inductance of HTS coil becomes the same as that of the normal coil.…”
Section: Inductance Of Hts Coilsupporting
confidence: 90%
See 1 more Smart Citation
“…At the very beginning, the inductance value of the HTS coil is about 90% of the normal one (108 mH for HTS coil and 118.9 mH for normal coil) and gradually increasing with the transport current, in agreement with previous findings [41]. Later, when the transport current reaches 11 A, the inductance of HTS coil becomes the same as that of the normal coil.…”
Section: Inductance Of Hts Coilsupporting
confidence: 90%
“…After validating the proposed modelling strategies and proving that the computation efficiency can be remarkably improved, there is one interesting finding that we would like to briefly discuss here. As concluded by previous work [41], the inductance of an HTS coil varies with the transport current, which can be explained by the non-uniform distribution of current in the tape. To be specific, for lower transport current, the current concentrates at the edge of the HTS tape and the inductance of the HTS coil is as small as 90% of the inductance of a normal conductor coil having the same geometry; then the inductance increases with the augmentation of transport current and becomes the same as that of the normal coil when transport current approaches the critical current of the HTS coil.…”
Section: Inductance Of Hts Coilmentioning
confidence: 76%
“…In more detail, the current densities concentrate on the upper and lower edges of the DP coil and exhibit a skin effect (see later in figure 6), and the skin effect becomes even more severe when the transport current is smaller or the current ramping rate is faster. So, the effective region of the HTS tapes to carry the current densities is narrowed to the upper and lower edges of the DP coil, leading to (1) the self and mutual inductances of the HTS tapes changing slightly [73][74][75]; (2) the effective resistance of the HTS tapes are increased, because the current densities are narrowed to concentrate in the effective region, leading to a smaller effective cross-sectional area of the superconducting wire and larger power-law resistivity.…”
Section: Model Validationmentioning
confidence: 99%
“…At high frequencies, the magnetic field coupling of the transformer coils is more complex, making the magnetic field distribution and current density of the coils difficult to calculate. Additionally, the variation of the current density in the superconducting coil makes the self-inductance of the superconducting coil not a constant value [16,17], and the metal reinforcement layer of the superconducting tape generates considerable eddy current losses at high frequencies [18][19][20]. Due to the special characteristics of superconducting coils at high frequencies, it is inaccurate to describe high frequency superconducting transformers with existing models.…”
Section: Introductionmentioning
confidence: 99%