. The Bell System technical journal . s: for a > I,V n = ±1, ^--^ 1 + (J 0 < (T < (70, n = ±l,i3 -; for (To < 0- 1, /i = — 1, and for 0 < cr < ao, = +1which correspond to /x and k both positive, the propagation constanttends to the value for a plane wave whose direction of circular polariza-tion coincides with that of the wave guide pattern. For o-o < o- < 1, \ i 1 - — /^ TE,, - MODES / / / / TE,2- MODES / /c xs/t > f / / - y / y / 10 ^ / ^ ^ z / ^ / ■ Fig. 13(f) — See Fig. 13. I i p = 0 \ P =0 ^,.^ ^
. The Bell System technical journal . s: for a > I,V n = ±1, ^--^ 1 + (J 0 < (T < (70, n = ±l,i3 -; for (To < 0- 1, /i = — 1, and for 0 < cr < ao, = +1which correspond to /x and k both positive, the propagation constanttends to the value for a plane wave whose direction of circular polariza-tion coincides with that of the wave guide pattern. For o-o < o- < 1, \ i 1 - — /^ TE,, - MODES / / / / TE,2- MODES / /c xs/t > f / / - y / y / 10 ^ / ^ ^ z / ^ / ■ Fig. 13(f) — See Fig. 13. I i p = 0 \ P =0 ^,.^ ^^VJ 7 / ^^ N, J / / / °^ \ ^ \ / -0. / / / / / / vs. / / .0 0 Fig. 13(g) —See Fig. 636 THE BELL SYSTEM TECHNICAL JOURNAL, MAY 1954. Fig. 13(h) —See Fig. 13.
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Keywords: ., bookcentury1900, bookdecade1920, booksubjecttechnology, bookyear1
