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Author's reply to “Comments on ‘Onsager–Casimir Principle and Reciprocity Relations for Bianisotropic Media’”

✍ Scribed by E. O. Kamenetskii


Publisher
John Wiley and Sons
Year
2001
Tongue
English
Weight
81 KB
Volume
31
Category
Article
ISSN
0895-2477

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✦ Synopsis


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 both the Lorentz adjointness relations and the macroscopic generalized reciprocity theorem can be derived, as usual, from the Onsager᎐Casimir principle, even in the most general case of a bianisotropic medium.


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Onsager–Casimir principle and reciprocit
✍ E. O. Kamenetskii 📂 Article 📅 1998 🏛 John Wiley and Sons 🌐 English ⚖ 122 KB 👁 1 views

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