他日关税重重
发表于 2025-3-25 05:04:15
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deadlock
发表于 2025-3-25 10:04:55
https://doi.org/10.1007/978-1-349-11612-6ime. The detailed properties of such free-fields were first studied in detail by Sherman, Devaney and Mandel [.], Sherman, Stamnes, Devaney and Lalor [.], and Devaney and Sherman [.] in the early 1970s. Such fields are of interest because they form the simplest type of wave phenomena encountered in both electromagnetics and optics.
极端的正确性
发表于 2025-3-25 13:25:01
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fatty-streak
发表于 2025-3-25 19:28:15
Kurt E. OughstunRigorous development of the classical microscopic Maxwell-Lorentz theory.Detailed development of the dipole radiation field from the Liénard-Wiechert potentials.Correlation of the microscopic and macr
Ascribe
发表于 2025-3-25 23:07:53
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睨视
发表于 2025-3-26 03:11:18
John E. Smith,P. Christopher Smith a dielectric waveguide) is a classical problem in both electromagnetics and optics. With Maxwell’s unifying theory [., .] of electromagnetism and optics, Lorentz’s classical model [.] of dielectric dispersion, and Einstein’s special theory of relativity [.], the stage was then set for a long-standi
fructose
发表于 2025-3-26 04:37:05
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深渊
发表于 2025-3-26 12:16:46
https://doi.org/10.1007/978-94-010-2828-8copic electric and magnetic field vectors that comprise the electromagnetic field. The analysis of the properties or the determination of an electromagnetic field is often facilitated by the introduction of auxiliary fields known as potentials. The two homogeneous Maxwell equations .·. = 0 and .×. =
Limousine
发表于 2025-3-26 14:25:17
,Hegelian ‘Organics’ and ‘Anthropology’,duce microscopic electric and magnetic fields. The microscopic equations of electromagnetics given in Eqs. (2.33)–(2.36) together with the Lorentz force relation given in Eq. (2.21) describe the detailed classical behavior of the charged particles and fields, as presented in Chapters 2 and 3. The ma
meditation
发表于 2025-3-26 20:36:35
https://doi.org/10.1007/978-3-476-02957-7dispersive media are developed in this chapter. The general frequency dependence of the dielectric permittivity, magnetic permeability, and electric conductivity is included in the analysis so that the resultant field equations rigorously apply to both perfect and imperfect dielectrics, conductors a