A constraint-based optimization technique for estimating physical parameters of Jiles – Atherton hysteresis model
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Published:2020-08-24
Issue:6
Volume:39
Page:1281-1298
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ISSN:0332-1649
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Container-title:COMPEL - The international journal for computation and mathematics in electrical and electronic engineering
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language:en
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Short-container-title:COMPEL
Author:
Upadhaya Brijesh,Rasilo Paavo,Perkkiö Lauri,Handgruber Paul,Belahcen Anouar,Arkkio Antero
Abstract
Purpose
Improperly fitted parameters for the Jiles–Atherton (JA) hysteresis model can lead to non-physical hysteresis loops when ferromagnetic materials are simulated. This can be remedied by including a proper physical constraint in the parameter-fitting optimization algorithm. This paper aims to implement the constraint in the meta-heuristic simulated annealing (SA) optimization and Nelder–Mead simplex (NMS) algorithms to find JA model parameters that yield a physical hysteresis loop. The quasi-static B(H)-characteristics of a non-oriented (NO) silicon steel sheet are simulated, using existing measurements from a single sheet tester. Hysteresis loops received from the JA model under modified logistic function and piecewise cubic spline fitted to the average M(H) curve are compared against the measured minor and major hysteresis loops.
Design/methodology/approach
A physical constraint takes into account the anhysteretic susceptibility at the origin. This helps in the optimization decision-making, whether to accept or reject randomly generated parameters at a given iteration step. A combination of global and local heuristic optimization methods is used to determine the parameters of the JA hysteresis model. First, the SA method is applied and after that the NMS method is used in the process.
Findings
The implementation of a physical constraint improves the robustness of the parameter fitting and leads to more physical hysteresis loops. Modeling the anhysteretic magnetization by a spline fitted to the average of a measured major hysteresis loop provides a significantly better fit with the data than using analytical functions for the purpose. The results show that a modified logistic function can be considered a suitable anhysteretic (analytical) function for the NO silicon steel used in this paper. At high magnitude excitations, the average M(H) curve yields the proper fitting with the measured hysteresis loop. However, the parameters valid for the major hysteresis loop do not produce proper fitting for minor hysteresis loops.
Originality/value
The physical constraint is added in the SA and NMS optimization algorithms. The optimization algorithms are taken from the GNU Scientific Library, which is available from the GNU project. The methods described in this paper can be applied to estimate the physical parameters of the JA hysteresis model, particularly for the unidirectional alternating B(H) characteristics of NO silicon steel.
Subject
Applied Mathematics,Electrical and Electronic Engineering,Computational Theory and Mathematics,Computer Science Applications
Reference50 articles.
1. Handbook of mathematical functions with formulas,1972
2. Parameter identification of the Jiles-Atherton hysteresis model using a hybrid technique;IET Electric Power Applications,2012
3. Identification of the Jiles-Atherton model parameters using simulated annealing method;Int. Conf. Elect. Mach. Syst. (ICEMS),2011
4. Comparison of Preisach and Jiles-Atherton models to take into account hysteresis phenomenon for finite element analysis;Journal of Magnetism and Magnetic Materials,2003
5. A simple vector generalization of the Jiles-Atherton model of hysteresis;IEEE Transactions on Magnetics,1996
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