2013
DOI: 10.1088/2040-8978/16/1/015701
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Energy density and velocity of electromagnetic waves in lossy chiral medium

Abstract: The average energy density of the macroscopic quasimonochromatic electromagnetic field U ts (t, r) in a linear passive chiral lossy medium described by the constitutive E-H relations is determined using a microscopic model. According to the model, U ts (t, r) is equal to the sum of the average energy densities of the electromagnetic field in free space U t0 (t, r) and electromagnetic oscillations in structural elements U s (t, r) induced by the electromagnetic wave. Making use of the Poynting theorem, the ener… Show more

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Cited by 13 publications
(27 citation statements)
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“…The quality-factor energy densities defined here are not circuit-model dependent [25,26] but depend only on the macroscopic constitutive parameters and fields of the antenna media (and thus are useful for antenna design). The Q-energy differs considerably from both the equivalent-circuit energy of Tretyakov [25,26] and the energy obtained by Vorobyev [27] in determining electromagnetic wave velocities in lossy dispersive material, but only slightly from the magnetic electrodynamic energy of Boardman and Marinov [28] in the frequency range where their magnetic energy is positive.…”
Section: General Expressions For Quality Factorcontrasting
confidence: 56%
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“…The quality-factor energy densities defined here are not circuit-model dependent [25,26] but depend only on the macroscopic constitutive parameters and fields of the antenna media (and thus are useful for antenna design). The Q-energy differs considerably from both the equivalent-circuit energy of Tretyakov [25,26] and the energy obtained by Vorobyev [27] in determining electromagnetic wave velocities in lossy dispersive material, but only slightly from the magnetic electrodynamic energy of Boardman and Marinov [28] in the frequency range where their magnetic energy is positive.…”
Section: General Expressions For Quality Factorcontrasting
confidence: 56%
“…Since the surface S a contains the equivalent electric and magnetic currents that reduce the fields to zero inside V a , one can divide E e into separate contributions, E e1 and E e2 , respectively, from electric and magnetic surface currents on S a ; that is, E e (r) = E e1 (r) + E e2 (r) (27) such that E e (r) ≈ 0 for r ∈ V a with the approximation becoming more accurate as ka gets smaller. In the far field, both E e1 and E e2 represent electric dipoles with dipole moments that can be designated as…”
Section: Minimization For the Quasi-static Electric Field Of The Elecmentioning
confidence: 99%
“…Energy density in lossy chiral media has been studied in recent papers [8][9][10]. These papers determine the energy density for the case of linear polarization and complement our studies, which focus on the effects of polarization selectivity of interaction with circularly polarized radiation in composites with helices of different shapes.…”
Section: Introductionmentioning
confidence: 75%
“…In comparison with the solutions obtained here, solutions from Ref. [10] cannot be used to study the pitch angle dependence and optimization of the electromagnetic properties of chiral media.…”
Section: Introductionmentioning
confidence: 85%
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