Titlebook: Electromagnetic Field Near Conducting Half-Space; Theory and Applicati Yuriy Vasetsky,Artur Zaporozhets Book 2024 The Editor(s) (if applica

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Cursory

Book 2024 field. These studies, unlike many well-known works, are based on obtained exact analytical solution of the problem for the field, generated by external current sources near the conducting body with plane surface. The solution for the vector and scalar potentials, electric and magnetic intensities i

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https://doi.org/10.1007/978-3-642-59228-7o the law of decrease field in conducting half-space is analyzed. It is shown, at the interface the expressions for the electric and magnetic intensities in the form of asymptotic series in addition to local field values of external sources contain their derivatives with respect to the coordinate pe

步兵

https://doi.org/10.1007/978-3-642-60943-5lsed electromagnetic fields the integrands are represented by bounded asymptotic series, in each term of which the dependences on coordinates and time are calculated separately using well-known simple expressions. Since the applied expansion into the asymptotic series is valid in the high-frequency

步兵

1876-1100 tensity perpendicular to the interface; the non-uniform electromagnetic field decreases in depth of conducting medium faster than uniform field). It is shown that the exact analytical solution depends on the va978-3-031-38425-7978-3-031-38423-3Series ISSN 1876-1100 Series E-ISSN 1876-1119

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過份艷麗

Electromagnetic Field of Arbitrary Spatial Current Contour Located Near Conducting Body with Flat S The analytical solutions for the vector and scalar potentials, electric and magnetic field intensities are defined both in dielectric and conducting media. The main feature of quasi-stationary electromagnetic field formation for system with plane interface between the dielectric and conducting medi

Hormones

Approximate Mathematical Models for Analysis of Alternating Electromagnetic Field of Sources Near Ckin effect is understood as its extended definition, when not only the penetration depth of the alternating field is small compared to the characteristic dimensions of the conducting body, but the ratio of the penetration depth to the characteristic dimensions of the entire electromagnetic system is