. The Bell System technical journal . ^^^ rX^ (b) 1 , ^t , , , - H OR E. Fig. 16—Fields of second stack mode in partially and completely filled planeClogston lines with mo = m, «o = «• 1158 THE BELL SYSTEM TECHNICAL JOURNAL, NOVEMBER 1952 these modes to the attenuation constant of the principal mode in acompletely filled Clogston 2. sf\a x« xzs (xw/t)2 (X33/t) M TT ¥2 TT % T 1 IT These results may be compared mth those given in Section IX forthe principal mode in plane Clogston lines having the same now to the cyl

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. The Bell System technical journal . ^^^ rX^ (b) 1 , ^t , , , - H OR E. Fig. 16—Fields of second stack mode in partially and completely filled planeClogston lines with mo = m, «o = «• 1158 THE BELL SYSTEM TECHNICAL JOURNAL, NOVEMBER 1952 these modes to the attenuation constant of the principal mode in acompletely filled Clogston 2. sf\a x« xzs (xw/t)2 (X33/t) M TT ¥2 TT % T 1 IT These results may be compared mth those given in Section IX forthe principal mode in plane Clogston lines having the same now to the cylindrical geometry, we remember that all thecircular transverse magnetic modes in a coaxial Clogston line N^ithinfinitesimally thin laminae and high-impedance boundaries are givenby the roots of equation (339) of Section IX, namely KoKo{koPi) -\- io3€oZiKi{Kopl) _ KoKaiKoPi) — icii€oZ2Kl{KoP2)Ko/o(koPi) — icO€oZiIi(KoPl) KoIo{K(iP2) + lOieoZ ol l{KoPi) (417)

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Keywords: ., bookcentury1900, bookdecade1920, booksubjecttechnology, bookyear1