{"title":"A Finite Element $a$-$h$-Formulation for the Reduced Order Hysteretic Magnetization Model for Composite Superconductors","authors":"Julien Dular;Arjan Verweij;Mariusz Wozniak","doi":"10.1109/TASC.2025.3528310","DOIUrl":null,"url":null,"abstract":"The simulation of transient effects in large-scale superconducting systems with the finite element method is computationally expensive. A Reduced Order Hysteretic Magnetization (ROHM) model has been recently proposed for the computation of the magnetization and loss of composite superconductors. It accounts for the interplay between hysteresis, eddy, and coupling effects, without a need to model the detailed current density distribution, leading to a substantial reduction of simulation time. The ROHM model naturally fits in finite element formulations written in terms of the magnetic field such as the <inline-formula><tex-math>$h$</tex-math></inline-formula>-<inline-formula><tex-math>$\\phi$</tex-math></inline-formula>- or <inline-formula><tex-math>$\\phi$</tex-math></inline-formula>-formulation, but these formulations are not always the optimal choice. For example, in the presence of ferromagnetic materials, one may prefer formulations written in terms of the magnetic flux density. In this context, we introduce in this paper a mixed <inline-formula><tex-math>$a$</tex-math></inline-formula>-<inline-formula><tex-math>$h$</tex-math></inline-formula>-formulation that implements the ROHM model. The main advantage of this formulation is the direct use of the constitutive relation defined by the ROHM model, without the need for its inversion. We discuss the computational efficiency of the new formulation compared to a conventional <inline-formula><tex-math>$\\phi$</tex-math></inline-formula>-formulation, based on a model of a composite superconducting strand.","PeriodicalId":13104,"journal":{"name":"IEEE Transactions on Applied Superconductivity","volume":"35 5","pages":"1-5"},"PeriodicalIF":1.7000,"publicationDate":"2025-01-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=10839043","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE Transactions on Applied Superconductivity","FirstCategoryId":"101","ListUrlMain":"https://ieeexplore.ieee.org/document/10839043/","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
引用次数: 0
Abstract
The simulation of transient effects in large-scale superconducting systems with the finite element method is computationally expensive. A Reduced Order Hysteretic Magnetization (ROHM) model has been recently proposed for the computation of the magnetization and loss of composite superconductors. It accounts for the interplay between hysteresis, eddy, and coupling effects, without a need to model the detailed current density distribution, leading to a substantial reduction of simulation time. The ROHM model naturally fits in finite element formulations written in terms of the magnetic field such as the $h$-$\phi$- or $\phi$-formulation, but these formulations are not always the optimal choice. For example, in the presence of ferromagnetic materials, one may prefer formulations written in terms of the magnetic flux density. In this context, we introduce in this paper a mixed $a$-$h$-formulation that implements the ROHM model. The main advantage of this formulation is the direct use of the constitutive relation defined by the ROHM model, without the need for its inversion. We discuss the computational efficiency of the new formulation compared to a conventional $\phi$-formulation, based on a model of a composite superconducting strand.
期刊介绍:
IEEE Transactions on Applied Superconductivity (TAS) contains articles on the applications of superconductivity and other relevant technology. Electronic applications include analog and digital circuits employing thin films and active devices such as Josephson junctions. Large scale applications include magnets for power applications such as motors and generators, for magnetic resonance, for accelerators, and cable applications such as power transmission.