在功率和音频频率下铁磁层磁特性的预先测定

O. Butler, C. Mang
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引用次数: 6

摘要

为了解释铁磁层在交流磁化作用下的行为的实验结果与经典解之间存在的差异,通过考虑磁导率和磁滞回线随最大磁通密度的变化在整个层层厚度上的变化,得到了一个更严格的解。为了分别研究基频和谐波频率的量,采用了谐波分析的方法来表示在任何时刻存在于层压截面上的毫米波和磁通密度之间的关系。确定总铁损耗的计算表明,在所涵盖的频率和磁通密度范围内,在施加电压的正弦波形或正弦激励电流的更常见的实际情况下,只需考虑基频的数量。与经典解相反,结果表明,即使通常的磁滞效应可以忽略不计,叠层中任何一点的磁通密度和磁通密度也不一定是同相的。因此,除了涡流和磁滞损耗的通常概念外,还会产生能量损失。对附加损耗存在的物理解释表明,它可以方便地称为微分迟滞损耗。铁损理论表达式的适用范围有一个上限,大约与磁化曲线的拐点相对应。对于超过这一点的磁化力值,提出了另一种解法。对Mumetal和硅钢样品进行了测试,以涵盖广泛的频率和磁通密度范围。在不引入渗透率虚拟值的情况下,由新公式计算出的理论损耗值占实测值的大部分。测量值和计算值的比较可以有效地表明材料的不均匀性。值得注意的是,层压厚度的减小会导致磁滞损耗的增加和磁导率的降低,磁导率的降低倾向于增加涡流损耗。这在低音频操作中尤其重要,因为层压厚度的减少会导致明显更高的总损耗。
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The predetermination of the magnetic properties of ferromagnetic laminae at power and audio frequencies
In order to explain the discrepancies which exist between results obtained experimentally and those determined from the classical solution of the behaviour of ferromagnetic laminae when subjected to a.c. magnetization, a more rigorous solution has been obtained by taking account of the variation of both the permeability and hysteresis loop, with changes in the maximum flux density, throughout the thickness of the lamination. A method of harmonic analysis has been utilized to represent the relationship which exists, at any instant of time, between the m.m.f. and flux density across the section of the lamination, in order that the quantities of fundamental and harmonic frequency may be separately investigated. Calculations to determine the total iron loss have shown that, for the range of frequency and flux density covered, only the quantities of fundamental frequency need be considered in the more usual practical case of sinusoidal waveform of applied voltage, or alternatively, of sinusoidal excitation current. Contrary to the classical solution, it is shown that the m.m.f. and flux density at any point in the lamination are not necessarily in phase, even when the usual hysteresis effect is negligible. In consequence, an energy loss occurs which is additional to the usual conception of eddy-current and hysteresis loss. The physical explanation of the existence of the additional loss suggests that it may conveniently be designated as the ?differential hysteresis loss.? The range of application of the theoretical expression for the iron loss is subject to an upper limit, corresponding approximately with the knee of the magnetization curve. An alternative solution is put forward for values of magnetizing force beyond this point. Tests have been carried out on samples of both Mumetal and silicon steel, to cover a wide range of frequencies and flux densities. The theoretical value of loss calculated from the new formulae accounts for the greater part of the measured value without introducing a fictitious value for the permeability. A comparison of the measured and calculated values gives a useful indication of the inhomogeneity of the material. It is noted that a reduction in lamination thickness results in an increase of the hysteresis loss and a reduction of the permeability, the latter effect tending to increase the eddy-current loss. This is of particular importance at low audio-frequency operation, where a reduction of lamination thickness can result in an appreciably higher total loss.
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