纳米晶材料
激发
介观物理学
粒度
物理
合金
核磁共振
算法
材料科学
凝聚态物理
计算机科学
量子力学
纳米技术
冶金
作者
Li Zhang,Yifan Wang,Liang Zou,Kaihang Guo,Yongjian Li,Qiuxia Sun
标识
DOI:10.1109/tmag.2023.3277075
摘要
To investigate the effects of internal microstructure and high-frequency non-sinusoidal excitation on the magnetic loss of nanocrystalline alloy, a three-dimensional mesoscopic model based on G. Herzer's theory of random anisotropy is developed.First, the AC test platform is used to measure the loss value of the nanocrystalline alloy under sinusoidal excitation, and then the model is subjected to the same excitation to obtain its loss value.These values are compared to verify the model's accuracy.Using the micromagnetic model provided by OOMMF software, we investigate the microscopic effect of grain size d on the high-frequency magnetic loss pv of nanocrystalline alloys.Next, we apply non-sinusoidal alternating magnetic fields (square wave, trapezoidal wave, and triangular wave) to the model to explore pv under non-sinusoidal excitation.The results show that as the grain size d of the nanocrystalline alloy increases, pv also increases.Additionally, when d and the frequency f are held constant, pv is greatest under triangular wave excitation, followed by trapezoidal wave excitation, and smallest under square wave excitation.This conclusion is due to the fact that the equivalent frequency feq, which contains the rate of change of magnetic flux density (dB/dt), can replace f in the Original Steinmetz Formula when the excitation source is non-sinusoidal.Our calculations indicate that feq is smaller under square wave excitation than under triangular wave excitation.
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