刘任, 顾朝阳, 孙江东, 唐波. Jiles-Atherton磁滞模型的改进与非正弦激励下软磁材料复杂磁滞准确模拟[J]. 中国电机工程学报, 2025, 45(5): 2016-2026. DOI: 10.13334/j.0258-8013.pcsee.231606
引用本文: 刘任, 顾朝阳, 孙江东, 唐波. Jiles-Atherton磁滞模型的改进与非正弦激励下软磁材料复杂磁滞准确模拟[J]. 中国电机工程学报, 2025, 45(5): 2016-2026. DOI: 10.13334/j.0258-8013.pcsee.231606
LIU Ren, GU Chaoyang, SUN Jiangdong, TANG Bo. Modified Jiles-Atherton Hysteresis Model and Accurate Simulation of Complex Hysteresis Characteristics of Soft Magnetic Materials Under Non-sinusoidal Excitation[J]. Proceedings of the CSEE, 2025, 45(5): 2016-2026. DOI: 10.13334/j.0258-8013.pcsee.231606
Citation: LIU Ren, GU Chaoyang, SUN Jiangdong, TANG Bo. Modified Jiles-Atherton Hysteresis Model and Accurate Simulation of Complex Hysteresis Characteristics of Soft Magnetic Materials Under Non-sinusoidal Excitation[J]. Proceedings of the CSEE, 2025, 45(5): 2016-2026. DOI: 10.13334/j.0258-8013.pcsee.231606

Jiles-Atherton磁滞模型的改进与非正弦激励下软磁材料复杂磁滞准确模拟

Modified Jiles-Atherton Hysteresis Model and Accurate Simulation of Complex Hysteresis Characteristics of Soft Magnetic Materials Under Non-sinusoidal Excitation

  • 摘要: 原始J-A(Jiles-Atherton)模型及其现有改进模型均不能准确模拟软磁材料在非正弦激励下含偏置小磁滞回环的复杂磁滞回线,因此,提出一种通用改进J-A模型已成为国际电磁场领域研究的热点与难点。为此,该文首先分析J-A模型不能准确模拟不同类型磁滞回环的问题,得到其根本原因为J-A模型中的不可逆磁化分量变化率未进行矫正,由此引入2个比例因子,控制其不可逆磁化分量满足要求;其次,发现J-A模型的钉扎系数和磁畴内耦合平均场参数随磁滞回线磁密幅值大小而变化,进一步提出改进J-A模型;另外,提出该改进模型参数的更新方法,弥补了传统方法须预知磁滞回线下一转折点数据的缺陷,需要指出的是,所提改进J-A模型所有参数通过实测对称磁滞回线即可辨识;最后,利用所提改进J-A模型与现有2种改进J-A模型分别模拟软磁材料在不同磁密下的对称磁滞回线与含偏置小回环的复杂磁滞回线,并对比实测值,验证所提改进J-A模型具有更高精度。

     

    Abstract: The original Jiles-Atherton (J-A) model and its existing improved models cannot accurately simulate the complex hysteresis loops embedded with biased minor loops, rendering the proposition of a universally applicable modified J-A model a challenging and popular research topic in the international electromagnetic field. In this paper, the fundamental reason why the J-A models cannot accurately simulate the different types of hysteresis loops is analyzed. It is found that the variation rate of irreversible magnetization component in J-A model should be corrected, and two scaling factors to control the variation of irreversible component are thus introduced. At the same time, the pinning coefficient and the mean-field coefficient of J-A model are found to vary with the magnetic induction of the simulated loop. A new modified J-A model is thus proposed. In addition, a new method of updating the modified J-A model parameters is proposed. This method addresses the inherent issue of traditional methods, which require prior knowledge of the next magnetization reversal point of the hysteresis loop. It should be pointed out that the parameters of proposed modified J-A model can be identified only by the measured symmetrical loops. Finally, the proposed and existing improved J-A models for simulating different types of hysteresis loops, i.e., symmetric hysteresis

     

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