2019
DOI: 10.1109/tasc.2019.2901874
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Numerical Model of HTS Cable and Its Electric-Thermal Properties

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Cited by 21 publications
(20 citation statements)
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“…where J C0 is the critical current density (A/m 2 ) at initial operating temperature T 0 = 70 (K) and the working magnetic field B (T ), T C is the critical temperature (K), a is the density exponent equal to 1.5 which is applicable to YBCO [28], I C0 is the self-field critical current per tape (A) at T 0 = 70, n tap is the number of HTS tapes and s HT S is the cross-sectional area of the superconductor. During the resistive state, when the temperature is above the critical value T C the current density of the HTS layer is reduced to 0.…”
Section: A Superconducting Cable Modelmentioning
confidence: 99%
“…where J C0 is the critical current density (A/m 2 ) at initial operating temperature T 0 = 70 (K) and the working magnetic field B (T ), T C is the critical temperature (K), a is the density exponent equal to 1.5 which is applicable to YBCO [28], I C0 is the self-field critical current per tape (A) at T 0 = 70, n tap is the number of HTS tapes and s HT S is the cross-sectional area of the superconductor. During the resistive state, when the temperature is above the critical value T C the current density of the HTS layer is reduced to 0.…”
Section: A Superconducting Cable Modelmentioning
confidence: 99%
“…where ๐ฝ ๐ถ,๐‘–๐‘› is the initial critical current density (๐ด/๐‘š 2 ) at initial temperature ๐‘‡ ๐‘œ = 70 ๐พ and at working magnetic field ๐ต, ๐‘‡ ๐ถ is the critical temperature (๐พ) and ๐‘Ž denotes the density exponent which is conventionally set to 1.5 for the YBCO material [8]. Based on (1), during the quenching process, as the temperature ๐‘‡(๐‘ก) increases, the value of the critical current density ๐ฝ ๐ถ decreases accordingly.…”
Section: Sc Modellingmentioning
confidence: 99%
“…where ๐ธ ๐ถ is the critical electric field equal to 1 ๐œ‡๐‘‰/๐‘๐‘š and the coefficient N has been set to 30 according to [8]. During the superconducting state, the resistivity of the HTS tapes is ๐œŒ ๐‘†๐ถ = 0 and the superconductor behaves as an ideal conductor.…”
Section: Sc Modellingmentioning
confidence: 99%
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“…Either finite element analysis (FEA) or finite-difference time-domain (FDTD) analysis of numerical models provides a valuable resource, as they remove multiple instances of creation and testing of hard prototypes for various high-fidelity situations. Various tools based on FEA and FDTD could be used for numerical models of HTS cables, such as MATLAB [15,16], ANSYS [17,18], COMSOL [19,20], etc. For time-dependent simulations such as fault analyses in the power system with HTS cables, the main limitation of numerical models based on FEM or FDTD is the computational burden.…”
Section: Introductionmentioning
confidence: 99%