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標題: Titlebook: Basic Electromagnetism; E. R. Dobbs Book 1993 E.R. Dobbs 1993 electricity.electromagnetic.electromagnetic wave.electromagnetism.electrosta [打印本頁]

作者: Negate    時間: 2025-3-21 19:43
書目名稱Basic Electromagnetism影響因子(影響力)




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書目名稱Basic Electromagnetism讀者反饋學(xué)科排名





作者: 評論者    時間: 2025-3-21 20:55
Electrostatics,until the eighteenth century when du Fay showed that there were two sorts of charge. One sort followed the rubbing of an amber rod with wool, the other a glass rod with silk. It was Benjamin Franklin who arbitrarily named the latter a positive charge and the original amber one a negative charge. He
作者: 運氣    時間: 2025-3-22 03:14
Electric potential and fields, important properties of a vector field are its flux and its circulation. For the electrostatic field these are expressed by integral equations (2.9) and (2.10) as follows:. In this chapter theorems from vector analysis are used to derive the differential forms of these equations and hence to descri
作者: 滋養(yǎng)    時間: 2025-3-22 06:22

作者: SPURN    時間: 2025-3-22 11:04

作者: cringe    時間: 2025-3-22 16:05

作者: deficiency    時間: 2025-3-22 18:51

作者: Acumen    時間: 2025-3-23 00:49
Electromagnetism and relativity,e can investigate the electric and magnetic fields of rapidly moving charges. Then by introducing a vector potential . subject to the Lorentz gauge condition we find a remarkable similarity between the equations of electrostatics, expressed in terms of the scalars . (potential) and ., and the equati
作者: 六邊形    時間: 2025-3-23 03:37

作者: 完整    時間: 2025-3-23 09:34

作者: urethritis    時間: 2025-3-23 12:12
Electromagnetic waves in conductors,teract with matter the largest effects come from the lightest charged particles, the electrons. In dielectrics the electrons are bound charges and in Chapter 10 we found that the polarization was characterized by the atomic polarizability . (.),given by the Clausius—Mossotti and Lorentz—Lorenz equat
作者: Obvious    時間: 2025-3-23 15:29

作者: 兇兆    時間: 2025-3-23 22:02
Michael W. Dunn,Michal Laniado-Schwartzmanroper understanding of the nature of matter. We shall therefore discuss dielectric behaviour in the chapter on electrostatics, conduction in metal wires in that on magnetostatics, and magnetism in matter (whether para-, dia- or ferro-magnetism) in the chapter on magnetism. In this first chapter the
作者: 匍匐    時間: 2025-3-24 00:39

作者: 訓(xùn)誡    時間: 2025-3-24 05:59

作者: Arboreal    時間: 2025-3-24 06:53
https://doi.org/10.1007/978-3-642-66763-3harges were of two types: free charges on conductors and fixed charges, arising from polarization, on dielectrics. We concluded our study by considering how elecrostatic fields could be used to focus a diverging beam of electrons in a vacuum. In this chapter we first discuss the nature of a steady e
作者: 抑制    時間: 2025-3-24 13:37

作者: abysmal    時間: 2025-3-24 15:13

作者: extract    時間: 2025-3-24 21:33

作者: Kidney-Failure    時間: 2025-3-25 03:00

作者: ESO    時間: 2025-3-25 06:02
Pathogenesis of Hemifacial Spasm,here are no conduction electrons, and (2) conductors. Many gases, liquids and solids are good dielectrics and we begin with the effects of an oscillating electric field on such dielectrics. We then solve Maxwell’s equations for linear, isotropic dielectrics and finally discuss the absorption and dis
作者: Curmudgeon    時間: 2025-3-25 10:23
Hemingway and the Spanish Civil Waris chapter we show that the wave properties of electromagnetic waves lead to the laws of reflection and refraction at plane surfaces, while their electromagnetic properties with the boundary conditions for electric and magnetic fields at dielectric interfaces lead to Fresnel’s equations for plane-po
作者: 意外的成功    時間: 2025-3-25 14:10
,Conspirators, January–February 1937,teract with matter the largest effects come from the lightest charged particles, the electrons. In dielectrics the electrons are bound charges and in Chapter 10 we found that the polarization was characterized by the atomic polarizability . (.),given by the Clausius—Mossotti and Lorentz—Lorenz equat
作者: Fluctuate    時間: 2025-3-25 18:31
https://doi.org/10.1007/978-3-030-19230-3 the question of their generation. Now we go back to the . and their solutions the .. We first develop these potentials for the radiant energy a long way from an oscillating electric dipole and then discuss how the radiators of electromagnetic energy at radio and microwave wavelengths (antennas) can
作者: Engaging    時間: 2025-3-25 21:47
Introduction,roper understanding of the nature of matter. We shall therefore discuss dielectric behaviour in the chapter on electrostatics, conduction in metal wires in that on magnetostatics, and magnetism in matter (whether para-, dia- or ferro-magnetism) in the chapter on magnetism. In this first chapter the nature of matter is summarized.
作者: Lacerate    時間: 2025-3-26 00:18

作者: CREST    時間: 2025-3-26 06:55

作者: 羊齒    時間: 2025-3-26 09:49
Michael W. Dunn,Michal Laniado-Schwartzmanroper understanding of the nature of matter. We shall therefore discuss dielectric behaviour in the chapter on electrostatics, conduction in metal wires in that on magnetostatics, and magnetism in matter (whether para-, dia- or ferro-magnetism) in the chapter on magnetism. In this first chapter the nature of matter is summarized.
作者: Prophylaxis    時間: 2025-3-26 16:34
Book 1993Professor Dobbs provides an elegant and clear account of thesubject, leading the student from electrostatics through to Maxwell‘sequations and electromagnetic waves, covering all the material neededby a student taking courses on electricity and magnetism andelectromagnetic waves.
作者: infatuation    時間: 2025-3-26 20:41
https://doi.org/10.1007/978-94-011-2112-5electricity; electromagnetic; electromagnetic wave; electromagnetism; electrostatics; fields; magnetic fie
作者: 機密    時間: 2025-3-26 21:40

作者: Aboveboard    時間: 2025-3-27 01:32
Guided waves,In this final chapter we consider first the difference between free space and guided waves and then develop the theory for electromagnetic waves in rectangular waveguides. A discussion of waveguide modes is followed by an introduction to resonant cavities and the chapter concludes with the shortcomings of the classical theory of cavity radiation.
作者: SPASM    時間: 2025-3-27 08:24

作者: 原始    時間: 2025-3-27 09:46

作者: Loathe    時間: 2025-3-27 14:37

作者: 青少年    時間: 2025-3-27 21:37
H. L. Rayner,B. A. Schacter,L. G. Israelsand (2.10) as follows:. In this chapter theorems from vector analysis are used to derive the differential forms of these equations and hence to describe the electric potentials and fields for a number of cases of practical importance.
作者: seroma    時間: 2025-3-28 01:17

作者: Consensus    時間: 2025-3-28 03:23

作者: Lime石灰    時間: 2025-3-28 06:34
Pathogenesis of Hemifacial Spasm,ing electric field on such dielectrics. We then solve Maxwell’s equations for linear, isotropic dielectrics and finally discuss the absorption and dispersion of electromagnetic waves in polar and non-polar dielectrics.
作者: 不可比擬    時間: 2025-3-28 13:59
Hemingway and the Spanish Civil Wartromagnetic properties with the boundary conditions for electric and magnetic fields at dielectric interfaces lead to Fresnel’s equations for plane-polarized waves. We conclude with a discussion of the special properties associated with waves incident at the Brewster angle and at angles greater than the critical angle.
作者: 土坯    時間: 2025-3-28 16:56

作者: 黃油沒有    時間: 2025-3-28 20:42
Electrostatics,r a glass rod with silk. It was Benjamin Franklin who arbitrarily named the latter a positive charge and the original amber one a negative charge. He also showed that the total charge in a rubbing experiment was constant.
作者: Fierce    時間: 2025-3-29 02:12
Electric potential and fields,and (2.10) as follows:. In this chapter theorems from vector analysis are used to derive the differential forms of these equations and hence to describe the electric potentials and fields for a number of cases of practical importance.
作者: inveigh    時間: 2025-3-29 05:06
Electromagnetism,ields to induced electric fields, from stationary to moving circuits. Electric and magnetic effects become intimately connected in the study of electromagnetism, which has already been introduced in the electromagnetic force equation (4.9) as . We first develop the concepts contained in Faraday’s law and then apply it to a variety of examples.
作者: Hemodialysis    時間: 2025-3-29 08:12
,Maxwell’s equations, relationships between the electric field . and the magnetic field . in the presence of electric charges and electric currents, whether steady or rapidly fluctuating, in a vacuum or in matter. These are ..
作者: 半導(dǎo)體    時間: 2025-3-29 14:57
Electromagnetic waves in dielectrics,ing electric field on such dielectrics. We then solve Maxwell’s equations for linear, isotropic dielectrics and finally discuss the absorption and dispersion of electromagnetic waves in polar and non-polar dielectrics.
作者: cunning    時間: 2025-3-29 18:21

作者: CALL    時間: 2025-3-29 22:24
Generation of electromagnetic waves,way from an oscillating electric dipole and then discuss how the radiators of electromagnetic energy at radio and microwave wavelengths (antennas) can be made directional. Finally we consider the classical scattering of electromagnetic waves.
作者: 厚顏    時間: 2025-3-30 03:51
Analysis and Reconstitution of Phytochromes,r . and . between two media. We continue with an introduction to each of the commonest types of magnetism, dia-, para- and ferromagnetism, and conclude by discussing the production of both permanent and powerful magnetic fields.
作者: PANIC    時間: 2025-3-30 04:39

作者: PRO    時間: 2025-3-30 09:09

作者: 兒童    時間: 2025-3-30 14:34
Electromagnetic waves in conductors,e densities of these carriers (Table 12.1) varies from 9 × 10. m . in a noble metal to about 10.–10. m . in semiconductors and dense plasmas, but can be as little as 10. m . in weakly ionized plasmas like the ionosphere, while interstellar gas has a density of about 10. m ..
作者: COLIC    時間: 2025-3-30 18:31
Magnetostatics,lectric current . in matter and introduce the concept of the magnetic field ., sometimes called the magnetic induction field. The relationships between steady or magnetostatic fields having ../. = 0 and steady or direct electric currents having ../. = 0 are then developed and illustrated with examples.
作者: 一窩小鳥    時間: 2025-3-30 21:21
Electromagnetism and relativity,ons of magnetostatics in terms of the vectors . and .. Finally we show, using a four-dimensional notation, that it is possible to reduce Maxwell’s four equations to just one equation which expresses directly the invariance of electromagnetism under the Lorentz transformation.
作者: FEIGN    時間: 2025-3-31 04:34
10樓
作者: 嚴峻考驗    時間: 2025-3-31 05:48
10樓




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