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Semianalytical method for the identification of inclusions by air-cored coil interaction in ferromagnetic media

机译:铁磁介质空气芯线圈相互作用鉴定夹杂物的半抗体方法

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The magnetostatic harmonic fields scattered by a near-surface air inclusion of arbitrary shape, embedded in a conductive ferromagnetic medium and illuminated by a current-carrying coil, are investigated. The scattering domain is separated into homogeneous subdomains under the assumption of a suitable truncation at a long distance from the incident source, whereas a perfect magnetic boundary condition is implied. The introduced methodology addresses the full coupling between the two interfaces, ie, the plane that distinguishes the half-space ferromagnetic material from the open air and the arbitrary surface among the inclusion and the ferromagnetic region. Therein, continuity conditions are applied in a rigorous way, while the expected behavior of the fields, either as ascending or as descending, are taken into account. The potentials associated with the half-space are expanded via cylindrical harmonic eigenfunctions, while those related with the inclusion's arbitrary geometry admit generalized-type formalism. However, since the transmission conditions involve potentials with different eigenexpansions, we are obliged to rewrite cylindrical to generalized functions and vice versa, obtaining handy relationships in terms of easy-to-handle integrals, where orthogonality then is feasible. Once done, the calculation of the exact solutions leads to infinite linear algebraic systems, manipulated through standard cut-off techniques. Thus, we obtain the implicated fields in a general analytical and compact fashion, independent of the inclusion's geometry. We demonstrate the efficiency of the analytical model approach, assuming the degenerate case of a spherical inclusion, whereas the air-cored coil simulation via a numerical procedure validates our method. The calculation is very fast, rendering it suitable for use with parametric inversion algorithms.
机译:研究了通过嵌入在导电铁磁介质中的近表面空气的近表面空气散射散射的磁谐谐波场,并通过携带电流携带线圈照射。散射结构域在距入射源的长距离的合适截短时分离成均匀子域,而暗示完美的磁边界条件。介绍的方法解决了两个接口之间的完全耦合,即,将半空间铁磁材料与夹持空气和夹杂物和铁磁区域之间的任意表面区分开的平面之间的完全耦合。其中,以严谨的方式应用连续性条件,而域的预期行为是升序或作为下降的。与半空间相关的电位通过圆柱形谐波特征断路来扩展,而与包含的任意几何形状相关的那些人承认广义式形式主义。然而,由于传输条件涉及具有不同特征的潜力,因此我们有义务将圆柱形重写为广义函数,反之亦然,并且在易于处理的积分方面获得方便的关系,其中正交性则是可行的。一旦完成,精确解决方案的计算导致无限的线性代数系统,通过标准截止技术操纵。因此,我们以一般的分析和紧凑的方式获得奇妙的字段,独立于包含的几何形状。我们展示了分析模型方法的效率,假设球形包含的简并含有,而通过数值过程的空气芯线圈仿真验证了我们的方法。计算非常快,呈现适用于参数反转算法。

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