3D simulations of total AC loss in a twisted multifilamentary MgB<sub>2</sub> wire carrying AC currents under AC magnetic fields at 20 K

Abstract In the pursuit of enabling the application of all-superconducting rotating machines in electric aviation, high AC loss in the armature windings where superconductors carry AC currents and exposed to AC/rotating magnetic fields is a critical stumbling block. For lowering AC loss, multifilamentary magnesium diboride (MgB 2 ) wires with fine filaments and tight twist are one promising candidate for aviation applications. In this paper, 3D AC loss simulations of a 54-filament MgB 2 wire with a non-magnetic matrix at 20 K are carried out based on the H -formulation. The transport loss carrying AC current without external field, Q t0 , of 12-, 30- and 54-filament wires is firstly obtained, where the current amplitudes range from 20% to 90% of its self-field critical current I c0 . Then the magnetization loss exposed to field amplitudes up to 2 T without current, Q m0 , is presented, where the operational frequency, the twist pitch and resistivity of the matrix are varied to investigate their impacts on Q m0 and its three loss components (hysteresis loss Q h , coupling loss Q c and eddy current loss Q e ). Lastly, the total loss, Q total , of the 54-filament wire with various twist pitches and frequencies is compared, where the current amplitudes vary from 30% to 70% of I c0 and the field amplitudes are up to 2 T. All simulations use the measured J c ( B , 20 K) and n ( B , 20 K) data of the 54-filament wire. Simulation results show that, the use of the 5 mm twist pitch wire can significantly reduce Q m0 due to the decoupling of the filaments, where the simulated Q h matches well with the analytical hysteresis loss for a cylindrical superconductor multiplied by 54 (the number of filaments). With increasing twist pitch, the filaments become coupled, resulting in a greater increase in both Q c and Q h . Surprisingly, the simulated Q total values in the wires with different twist pitches agree well with the sum of Q m0 and Q t0 for all different current levels. This implies that Q total in an MgB 2 wire carrying an AC current exposed to an AC magnetic field can be accurately predicted by knowing Q m0 and Q t0 values which are more easily obtained.

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Publication Details

Journal
Superconductor Science and Technology
Published
2025-05-01
DOI
https://doi.org/10.1088/1361-6668/add42a
Citations
4
Primary Topic
Superconductivity in MgB2 and Alloys
Type
article
Field-Weighted Citation Impact
5.03

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article

3D simulations of total AC loss in a twisted multifilamentary MgB2 wire carrying AC currents under AC magnetic fields at 20 K

Zhenan Jiang, Rodney A. Badcock, Mark Ainslie, Nick Strickland et al.
4 citations
Superconductor Science and Technology
Superconductivity in MgB2 and Alloys
5.03
article

3D simulations of total AC loss in a twisted multifilamentary MgB2 wire carrying AC currents under AC magnetic fields at 20 K

Zhenan Jiang, Rodney A. Badcock, Mark Ainslie, Nick Strickland, Yueming Sun, Yukai Qiao, Matthew Rindfleisch
article en
4 citations

Abstract

Abstract In the pursuit of enabling the application of all-superconducting rotating machines in electric aviation, high AC loss in the armature windings where superconductors carry AC currents and exposed to AC/rotating magnetic fields is a critical stumbling block. For lowering AC loss, multifilamentary magnesium diboride (MgB 2 ) wires with fine filaments and tight twist are one promising candidate for aviation applications. In this paper, 3D AC loss simulations of a 54-filament MgB 2 wire with a non-magnetic matrix at 20 K are carried out based on the H -formulation. The transport loss carrying AC current without external field, Q t0 , of 12-, 30- and 54-filament wires is firstly obtained, where the current amplitudes range from 20% to 90% of its self-field critical current I c0 . Then the magnetization loss exposed to field amplitudes up to 2 T without current, Q m0 , is presented, where the operational frequency, the twist pitch and resistivity of the matrix are varied to investigate their impacts on Q m0 and its three loss components (hysteresis loss Q h , coupling loss Q c and eddy current loss Q e ). Lastly, the total loss, Q total , of the 54-filament wire with various twist pitches and frequencies is compared, where the current amplitudes vary from 30% to 70% of I c0 and the field amplitudes are up to 2 T. All simulations use the measured J c ( B , 20 K) and n ( B , 20 K) data of the 54-filament wire. Simulation results show that, the use of the 5 mm twist pitch wire can significantly reduce Q m0 due to the decoupling of the filaments, where the simulated Q h matches well with the analytical hysteresis loss for a cylindrical superconductor multiplied by 54 (the number of filaments). With increasing twist pitch, the filaments become coupled, resulting in a greater increase in both Q c and Q h . Surprisingly, the simulated Q total values in the wires with different twist pitches agree well with the sum of Q m0 and Q t0 for all different current levels. This implies that Q total in an MgB 2 wire carrying an AC current exposed to an AC magnetic field can be accurately predicted by knowing Q m0 and Q t0 values which are more easily obtained.

Superconductor Science and TechnologyVol. 38(5)
King's College London (GB), Victoria University of Wellington (NZ), Hyper Tech Research (United States) (US)
Ministry of Business, Innovation and Employment, China Scholarship Council
Openalex Percentile: Top 5%
Superconductivity in MgB2 and Alloys
5.03
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