Advanced magnetic hysteresis model describing polarization and frequency dependence

C. Freitag, T. Leibfried
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引用次数: 1

Abstract

In this paper a hysteresis model for electrical steel based on a numerical Fourier expansion of the magnetic field as function of magnetic polarization and frequency is proposed. The model setup relies on measured data. A single sheet tester is used for gauging hysteresis curves from minor to major loops with a frequency range starting at 50 Hz up to 250 Hz. The polarization is controlled to be cosinusoidal, as required by the standard IEC 60404-3. Whereas the magnetic polarization has a cosine waveform the corresponding magnetic field has a non-sinusoidal waveform. As a matter of the non-linear dependence between polarization and field, all harmonics are part of the magnetic field. A Fourier analysis of the magnetic field delivers harmonics as summation of cosine and sine waves. Two relationships can be found: one between the amplitudes of these waves and the amplitude of the polarization and another between the amplitudes of these waves and the frequency of the polarization. They are described via cubic spline interpolation. With an interpolation for each harmonic, the magnetic field is created as a sum of cosine and sine functions. Measured and modeled hysteresis loops are compared. The error of the model is determined. Finally, a hysteresis model for electrical steel is developed which is able to calculate a magnetic field for arbitrary polarization amplitudes and frequencies. Measured and modeled hysteresis loops are compared. The error of the model is determined. Finally, a hysteresis model for electrical steel is developed which is able to calculate a magnetic field for arbitrary polarization amplitudes and frequencies.
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描述极化和频率依赖关系的先进磁滞模型
本文提出了一种基于磁场随磁极和频率的数值傅里叶展开的电工钢磁滞模型。模型的建立依赖于测量数据。单片测试仪用于测量从小回路到大回路的滞后曲线,频率范围从50 Hz到250 Hz。根据标准IEC 60404-3的要求,极化被控制为余弦。磁极化具有余弦波形,而相应的磁场具有非正弦波形。由于极化与场之间的非线性关系,所有的谐波都是磁场的一部分。磁场的傅里叶分析将谐波作为余弦和正弦波的总和。可以发现两种关系:一种是这些波的振幅和极化的振幅之间的关系,另一种是这些波的振幅和极化的频率之间的关系。它们通过三次样条插值来描述。通过对每个谐波的插值,磁场被创建为余弦和正弦函数的和。比较了实测和模拟的磁滞回线。确定了模型的误差。最后,建立了电工钢的磁滞模型,该模型能够计算任意极化幅值和频率下的磁场。比较了实测和模拟的磁滞回线。确定了模型的误差。最后,建立了电工钢的磁滞模型,该模型能够计算任意极化幅值和频率下的磁场。
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