考虑动态磁损耗的铁氧体铁芯电感电路仿真模型

H. Saotome, Y. Hamamoto, K. Azuma
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引用次数: 4

摘要

本研究的目的是建立用于电源变换器的铁氧体电感和变压器的精确损耗电路仿真模型。铁氧体的功率损耗主要是磁滞损耗和动态磁损耗。随着激励频率的降低,B-H回路变窄。然而,即使在低于1khz的频率下,B-H回路也表现出一定的最小宽度。这个回路被称为直流迟滞回路或简称为迟滞回路。动态磁损耗是通过减去在1 - 10khz以上频率测量的B-H回路面积的磁滞损耗得到的。引起动态磁损耗的磁场强度Hf定义为(dB/dt)A, f,其中kf为动态磁损耗参数。在矩形波形电压激励下,从测量的B- h回路得到Hf作为B和dB/dt的函数。利用高频数据,模拟了正弦波形电压激励下dB/dt瞬时值随时间变化的B- H回路。仿真结果与实验结果吻合较好。本研究的结果有助于建立铁氧体应用磁性器件的精确损耗非线性仿真电路模型。该模型可用于电力电子器件的设计。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Circuit simulation model for ferrite core inductor taking into account dynamic magnetic loss
The purpose of this study is to develop a precise-loss circuit simulation model for ferrite inductors and transformers used in power converters. The power loss in ferrite is mainly due to the magnetic losses of hysteresis and dynamic magnetic losses. The B-H loop becomes narrower with decreasing excitation frequency. However, even at frequencies lower than 1 kHz, the B-H loop exhibits a certain minimum width. This loop is referred to as the DC hysteresis loop or simply the hysteresis loop. The dynamic magnetic loss is obtained by subtracting the hysteresis loss from the B-H loop area measured at a frequency above 1–10 kHz. Magnetic field intensity, Hf, causing the dynamic magnetic loss is defined as (dB/dt)A, f, where kf is the dynamic magnetic loss parameter. Hf is obtained as a function of B and dB/dt from the measured B-H loops under rectangular waveform voltage excitation. Using the Hf data, we simulated B- H loops under sinusoidal waveform voltage excitation where the instantaneous value of dB/dt changes at every moment in time. The simulated and experimental results were in good agreement. The results of the present study contribute to the development of a precise-loss nonlinear simulation circuit model for ferrite-applied magnetic devices. The model can be used in the design of power electronics.
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