and it is apparent that 15 ᎐ 18 are equivalent to 3 ᎐ 5 . Therefore, there is no difference between the ''dynamical w Ž .x constitutive symmetry relations,'' summarized in 1, eq. 6 , Ž . Ž . and the Lorentz adjointness 3 ᎐ 5 . Since these two set of relations are equivalent, we can conclude that bot
Comments on “Onsager–Casimir Principle and Reciprocity Relations for Bianisotropic Media”
✍ Scribed by R. Marqués
- Publisher
- John Wiley and Sons
- Year
- 2001
- Tongue
- English
- Weight
- 72 KB
- Volume
- 31
- Category
- Article
- ISSN
- 0895-2477
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📜 SIMILAR VOLUMES
To use the general reciprocity theorem for bianisotropic media, the physical basis should be established. There is the Onsager᎐Casimir principle that shows how the time-re¨ersal in¨ariance of microscopic equations of motion gi¨es certain relations for macroscopic susceptibilities of a causal linear
The claim of Liu et al. in a recent paper in this journal that rigor is lacking and something is amiss in pre¨iously deri¨ed expressions of the infinite-medium dyadic Green's functions of a homogeneous, isotropic chiral medium is shown to be without any substance. As a consequence, the paper by Liu
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