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Titlebook: Electrodynamics of Magnetoactive Media; I. D. Vagner,B. I. Lembrikov,P. Wyder Book 2004 Springer-Verlag Berlin Heidelberg 2004 Electrodyna

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發(fā)表于 2025-3-21 16:22:10 | 只看該作者 |倒序瀏覽 |閱讀模式
書目名稱Electrodynamics of Magnetoactive Media
編輯I. D. Vagner,B. I. Lembrikov,P. Wyder
視頻videohttp://file.papertrans.cn/306/305939/305939.mp4
概述First book on this topic with textbook potential
叢書名稱Springer Series in Solid-State Sciences
圖書封面Titlebook: Electrodynamics of Magnetoactive Media;  I. D. Vagner,B. I. Lembrikov,P. Wyder Book 2004 Springer-Verlag Berlin Heidelberg 2004 Electrodyna
描述Our objective was primarily to consider in a separate treatise from the general point of view a theory of as many electrodynamic phenomena in a magnetic field as possible. The choice of material was determined by both the ab- sence of such a book and the scientific interests of the authors. From the very beginning, however, we felt it necessary to include the fundamentals of electrodynamics that are required for the thorough analysis of particular processes. We believe that it is convenient for a reader to find in the same book a consistent review of some special fields in physics and a complete set of theoretical instruments that are necessary for the clear understanding of more advanced parts of the book. There exists a number of excellent textbooks and monographs describing the problems of classical electrodynamics in general and its applications to continuous media. We have to acknowledge, for example, the following funda- mental books: Electrodynamics by A. Sommerfeld [1], The Classical Theory of Fields by L.D. Landau and E.M. Lifshitz [2], Electromagnetic Theory by J.A. Stratton [3], and Electrodynamics of Continuous Media by L.D. Lan- dau and E.M. Lifshitz [4]. This list is
出版日期Book 2004
關(guān)鍵詞Electrodynamics; Electromagnetic phenomena; Electromagnetic waves; Maxwell‘s equations; Plasma; Supercond
版次1
doihttps://doi.org/10.1007/978-3-662-06941-7
isbn_softcover978-3-642-07825-5
isbn_ebook978-3-662-06941-7Series ISSN 0171-1873 Series E-ISSN 2197-4179
issn_series 0171-1873
copyrightSpringer-Verlag Berlin Heidelberg 2004
The information of publication is updating

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發(fā)表于 2025-3-21 22:31:43 | 只看該作者
Quasi-static Electromagnetic Field,nt external magnetic field. The field and current variations are assumed to be sufficiently slow such that the field distribution at any moment of time can be described as static and created by the currents existing at this moment.
板凳
發(fā)表于 2025-3-22 00:26:58 | 只看該作者
Electromagnetic Waves,equencies small compared to the eigenfrequencies of the molecular and electronic oscillations. Then the material equations, i.e. the relations between the vectors . and ., and . and . remain the same as in the case of the constant fields.
地板
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5#
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Waves in Plasma,ion and expressions for the current density for each type of charged particles. The longitudinal quasi-static electric field caused by charge carriers oscillations has been determined by the Poisson equation. However, this approach is inadequate for the study of electromagnetic wave propagation in p
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Book 2004ic field as possible. The choice of material was determined by both the ab- sence of such a book and the scientific interests of the authors. From the very beginning, however, we felt it necessary to include the fundamentals of electrodynamics that are required for the thorough analysis of particula
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發(fā)表于 2025-3-23 04:24:08 | 只看該作者
Current Instabilities,ed as stable, if these deviations do not increase with time, and in such a case the system cannot function as an oscillator or amplifier. In the opposite case, when the small deviations increase with time, the system is unstable, and it can be used as an oscillator or amplifier. In the further analysis we mainly follow [11,12].
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發(fā)表于 2025-3-23 09:02:53 | 只看該作者
Ingrid Gogolin,Antje Hansen,Dominique Rauchcan be either positive, or negative. It can be measured and has its own dimension. In the MKS system of units which is used in this book the unit of an electric charge is .. The charge of an electron is, as it is well known, negative, and its absolute value e is 1.60 × 10. coulomb.
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