A new benchmark problem for electromagnetic modelling of superconductors: the high-T c superconducting dynamo

发电机 水准点(测量) 超导磁体 导线 超导电性 导电体 物理 磁铁 电压 计算机科学 机械 磁场 统计物理学 计算物理学 拓扑(电路) 凝聚态物理 电气工程 数学 几何学 大地测量学 工程类 量子力学 地理
作者
Mark Ainslie,Francesco Grilli,Loïc Quéval,Enric Pardo,Fernando Perez-Mendez,Ratu Mataira,Antonio Morandi,Asef Ghabeli,Chris W. Bumby,Roberto Brambilla
出处
期刊:Superconductor Science and Technology [IOP Publishing]
卷期号:33 (10): 105009-105009 被引量:60
标识
DOI:10.1088/1361-6668/abae04
摘要

The high-Tc superconducting (HTS) dynamo is a promising device that can inject large DC supercurrents into a closed superconducting circuit. This is particularly attractive to energise HTS coils in NMR/MRI magnets and superconducting rotating machines without the need for connection to a power supply via current leads. It is only very recently that quantitatively accurate, predictive models have been developed which are capable of analysing HTS dynamos and explain their underlying physical mechanism. In this work, we propose to use the HTS dynamo as a new benchmark problem for the HTS modelling community. The benchmark geometry consists of a permanent magnet rotating past a stationary HTS coated-conductor wire in the open-circuit configuration, assuming for simplicity the 2D (infinitely long) case. Despite this geometric simplicity the solution is complex, comprising time-varying spatially-inhomogeneous currents and fields throughout the superconducting volume. In this work, this benchmark problem has been implemented using several different methods, including H-formulation-based methods, coupled H-A and T-A formulations, the Minimum Electromagnetic Entropy Production method, and integral equation and volume integral equation-based equivalent circuit methods. Each of these approaches show excellent qualitative and quantitative agreement for the open-circuit equivalent instantaneous voltage and the cumulative time-averaged equivalent voltage, as well as the current density and electric field distributions within the HTS wire at key positions during the magnet transit. A critical analysis and comparison of each of the modelling frameworks is presented, based on the following key metrics: number of mesh elements in the HTS wire, total number of mesh elements in the model, number of degrees of freedom (DOFs), tolerance settings and the approximate time taken per cycle for each model.
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