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Electrical circuit models of the HF initial permeability spectra of soft ferrite lead to revised definition of fundamental material properties

机译:软铁氧体的HF初始磁导率谱的电路模型导致基本材料性能的修订定义

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Engineers are usually interested in the relative magnetic permeability of a soft ferrite μr, whereas physicists and material scientists are more interested in the magnetic susceptibility χ. The magnetostatic relationship between these dimensionless scalars is simply μr = χ+1. But ferrite for HF must be considered in magnetodynamic terms. The simplest physical approach to this is to apply Debye's mathematical model of simple relaxation. This gives an expression for the complex susceptibility spectrum χ(ω), in which the imaginary term represents the loss. However, complex susceptibility and permeability can be expressed in either series or parallel terms, the latter having primacy. Electrical circuit models show that we cannot conclude that μr(ω) = χ(ω)+1. This leads to a clarification of the relationship between the susceptibility and permeability in the presence of loss. A parallel model for the initial permeability spectra of ferrites is presented, the variables being the static susceptibility, Snoek's Product and the maximum Q. The relative loss factor, tanδm/μi is shown to be an approximation for the reciprocal of the imaginary part of the parallel permeability.
机译:工程师通常对软铁氧体μr的相对磁导率感兴趣,而物理学家和材料科学家对磁化率χ更感兴趣。这些无量纲标量之间的静磁关系仅为μr=χ+ 1。但是,必须从磁动力学角度考虑用于HF的铁氧体。最简单的物理方法是应用Debye的简单松弛数学模型。这给出了复磁化率谱χ(ω)的表达式,其中虚项表示损耗。但是,复杂的磁化率和磁导率可以用串行或并行术语表示,后者具有首要地位。电路模型表明,我们不能得出μr(ω)=χ(ω)+1的结论。这导致在存在损失的情况下磁化率和磁导率之间关系的澄清。给出了铁氧体初始磁导率谱的并行模型,变量为静态磁化率,Snoek积和最大Q。相对损耗因子tanδm/μi显示为铁氧体虚部倒数的近似值。平行磁导率。

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