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Enhancement of electrocaloric response and elevated energy-storage characteristics in lead-free BCTZ-ZN ceramics. [PDF]
RSC AdvAbdmouleh H +4 more
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Density-functional tight binding meets Maxwell: unraveling the mysteries of (strong) light-matter coupling efficiently. [PDF]
NanophotonicsSidler D +5 more
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Design and numerical analysis of high contrast ratio and ultra-compact all-optical 2-bit reversible comparator. [PDF]
HeliyonVeisi E, Seifouri M, Olyaee S.
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, 2022 Maxwellove jednadžbe temeljne su jednadžbe elektromagnetizma, koje kombiniraju Gaussov zakon elektriciteta, Faradayev zakon elektromagnetske indukcije, Gaussov zakon magnetizma i Ampèreov zakon struje u vodiču.
Kondić, Jelena
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On the derivation of Maxwell's equations
Physics Letters, 1964Maxwell's equations in material media can be derived from (~ electron theory ~> in two steps. First, from the electromagnetic equations for fields with point sources (electrons and nuclei), valid at what we shall call the steb-atomic lecel, the equations, which take into account the existence of stable atoms, molecules o1" ions must he derived.
de Groot, S. R., Vlieger, J.
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ON THE HOMOGENIZATION OF MAXWELL EQUATIONS
COMPEL - The international journal for computation and mathematics in electrical and electronic engineering, 1995We discuss the following general problem: given a composite, made from at least two different materials with each its own (scalar, and possibly complex‐valued) ε and μ, distributed in space in a regular, crystal‐like, pattern, find the equivalent permittivity and permeability (they will, in general, be tensors). This is homogenization. A computation in
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On the strength of Maxwell’s equations
Journal of Mathematical Physics, 1987The ‘‘strength’’ of a set of field equations (first defined by Einstein as the number of Taylor coefficients of field variables that could be chosen arbitrarily) is used to show that the amount of initial data required by the electromagnetic formulation of Maxwell’s theory in free space is equal, without approximation, to that required by the potential
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2014
This chapter is devoted to the review of Maxwell’s equations in differential and integral forms as well as the electromagnetic boundary conditions. We will also discuss the electromagnetic potentials and wave equations. The solution to inhomogeneous wave equation using field representations by the Green’s function will be presented.
Kasra Barkeshli, Sina Khorasani
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This chapter is devoted to the review of Maxwell’s equations in differential and integral forms as well as the electromagnetic boundary conditions. We will also discuss the electromagnetic potentials and wave equations. The solution to inhomogeneous wave equation using field representations by the Green’s function will be presented.
Kasra Barkeshli, Sina Khorasani
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2021
Since Maxwell established a foundation of the modern electromagnetic theory in 1873 [1], electromagnetics has undergone a rapid development and has been one of the most important research areas in engineering and science. It demands the study of Maxwell’s equations and their application to the analysis and design of devices and systems.
Gang Bao, Peijun Li
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Since Maxwell established a foundation of the modern electromagnetic theory in 1873 [1], electromagnetics has undergone a rapid development and has been one of the most important research areas in engineering and science. It demands the study of Maxwell’s equations and their application to the analysis and design of devices and systems.
Gang Bao, Peijun Li
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1996
Abstract The field equations for the general. time-varying case are collectively known as Maxwell’s equations after J C. Maxwell. Several results were obtained by Ampere, Faraday, Gauss and Coulomb Thus Maxwell’s equations are the culmination of many years of research into the electric and magnetic phenomena.
P Neittaanmäki, M Rudnicki, A Savini
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Abstract The field equations for the general. time-varying case are collectively known as Maxwell’s equations after J C. Maxwell. Several results were obtained by Ampere, Faraday, Gauss and Coulomb Thus Maxwell’s equations are the culmination of many years of research into the electric and magnetic phenomena.
P Neittaanmäki, M Rudnicki, A Savini
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