Material models can be classified into physical and phenomenological models. Phenomenological models are constructed by fitting model parameters to measured data. They are determined using as few measured data as possible, but it is generally difficult for phenomenological models to predict material properties under conditions outside the measured data. In contrast, physical models can theoretically predict material properties based only on basic material constants. In this talk, after efficient and accurate phenomenological models are introduced, a physical model of magnetic materials is discussed.
The play model is a powerful phenomenological model. Its scalar model is mathematically equivalent to the classical Preisach model. It allows both the magnetic field and the flux density as its input to accurately describe the hysteretic property. The play model can be vectorized to construct an efficient vector hysteresis model [1], [2]. By combining the play model with a Cauer circuit, an accurate dynamic hysteresis model can be constructed [3]. Figure 1(a) shows simulated BH loops under PWM excitation, where the loops and losses are accurately reconstructed.
The development of a physical material model is a challenging task because of the multiscale nature of magnetic materials, where domain-wall behavior at the nm scale affects macroscopic properties at the mm/cm scale. Based on mesoscopic magnetic-domain modeling at the crystal-grain scale, a physical multiscale model of magnetic material was developed [4], [5]. It is an energy-based model that can handle the influence of physical factors in their energy forms. For example, magneto-mechanical interactions can be included by adding magneto-elastic energy. The multi-scale model successfully predicted stress-dependent properties of silicon steel [Fig. 1(b)].
Fig. 1 Simulation results of non-oriented silicon steel: (a) BH loops under PWM excitation given by a phenomenological model and (b) stress dependence of hysteresis loss predicted by a physical model.
References:
[1] T Matsuo, “Anisotropic vector hysteresis model using an isotropic vector play model,” IEEE Trans. Magn., vol. 46, pp. 3041-3044, 2010.
[2] T Matsuo, M Miyamoto, “Dynamic and anisotropic vector hysteresis model based on isotropic vector play model for nonoriented silicon steel sheet,” IEEE Trans. Magn., vol. 48, pp. 215-218, 2012.
[3] Y. Shindo, T. Miyazaki, T. Matsuo, “Cauer circuit representation of the homogenized eddy-current field based on the Legendre expansion for a magnetic sheet,” IEEE Trans. Magn., vol. 52, 6300504, 2016.
[4] S. Ito, T. Mifune, T. Matsuo, C. Kaido, Y. Takahashi, K. Fujiwara, “Simulation of the stress dependence of hysteresis loss using an energy-based domain model,” AIP Advances, vol. 8, 047501, 2018.
[5] T. Matsuo, Y. Takahashi, K. Fujiwara, “Pinning field model using play hysterons for stress-dependent domain-structure model,” J. Magn. Magn. Mater., vol. 499, 166303, 2020.