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Area Transmission lines and waveguides / Polarization of waves and fields

IEV ref 726-04-16

en
orthogonal modes
two modes for which the total power crossing any transverse cross-section is equal to the total flux, through that cross-section, of the sum of the individual Poynting vectors of the modes; in other terms, the total flux across that cross-section, of the sum of the two cross-products E 1 × H 2 + E 2 × H 1 MathType@MTEF@5@5@+=feaagCart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbbjxAHXgarqqtubsr4rNCHbGeaGqipG0dh9qqWrVepG0dbbL8F4rqqrVepeea0xe9LqFf0xc9q8qqaqFn0lXdHiVcFbIOFHK8Feea0dXdar=Jb9hs0dXdHuk9fr=xfr=xfrpeWZqaaeqabiGaciGacaqadmaadaqaaqaaaOqaaiqadweagaWcamaaBaaaleaacaaIXaaabeaakiabgEna0kqadIeagaWcamaaBaaaleaacaaIYaaabeaakiabgUcaRiqadweagaWcamaaBaaaleaacaaIYaaabeaakiabgEna0kqadIeagaWcamaaBaaaleaacaaIXaaabeaaaaa@418F@ in the total Poynting vector, is zero

fr
modes orthogonaux, m pl
couple de modes pour lesquels la puissance totale traversant une section droite est égale au flux total à travers cette surface de la somme des vecteurs de Poynting de chaque mode; en d'autres termes, le flux total à travers cette section droite, de la somme des deux produits croisés E 1 × H 2 + E 2 × H 1 MathType@MTEF@5@5@+=feaagCart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbbjxAHXgarqqtubsr4rNCHbGeaGqipG0dh9qqWrVepG0dbbL8F4rqqrVepeea0xe9LqFf0xc9q8qqaqFn0lXdHiVcFbIOFHK8Feea0dXdar=Jb9hs0dXdHuk9fr=xfr=xfrpeWZqaaeqabiGaciGacaqadmaadaqaaqaaaOqaaiqadweagaWcamaaBaaaleaacaaIXaaabeaakiabgEna0kqadIeagaWcamaaBaaaleaacaaIYaaabeaakiabgUcaRiqadweagaWcamaaBaaaleaacaaIYaaabeaakiabgEna0kqadIeagaWcamaaBaaaleaacaaIXaaabeaaaaa@418F@ dans le vecteur de Poynting total, est nulle

ar
أنماط متعامدة

de
orthogonale Moden, m, pl

es
modos ortogonales

fi
ortogonaaliset aaltomuodot

it
modi ortogonali

ko
직교 모드

ja
直交モード

pl
rodzaje ortogonalne (pola)

pt
modos ortogonais

sv
ortogonala moder

Publication date: 1982
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