. The Bell System technical journal . Fig. 13—Fields of principal mode in partiallj^ and completely filled planeClogston lines with mo = m, to = «. LAMINATED TRANSMISSION LINES. II 1141 tioiis may easily be obtained, if desired, from the expressions for thefield components. As a numerical example we have plotted in Fig. 13 the fields of theprincipal mode for plane transmission lines in which the stacks fillrespectively one-quarter, one-half, three-quarters, and all of the totalavailable space. For simplicity we have taken /xo = ji, eo = e, and nor-malized the fields so that the total one-way c
. The Bell System technical journal . Fig. 13—Fields of principal mode in partiallj^ and completely filled planeClogston lines with mo = m, to = «. LAMINATED TRANSMISSION LINES. II 1141 tioiis may easily be obtained, if desired, from the expressions for thefield components. As a numerical example we have plotted in Fig. 13 the fields of theprincipal mode for plane transmission lines in which the stacks fillrespectively one-quarter, one-half, three-quarters, and all of the totalavailable space. For simplicity we have taken /xo = ji, eo = e, and nor-malized the fields so that the total one-way current is the same in allfour cases. The average current density is of course gEz in the stacksand zero in the main dielectric. The first case approximates most nearlyto the extreme Clogston 1 line discussed in Part I, while the last caseis the complete Clogston 2, and the intermediate cases show the transi-tion between these two structures. The following table gives xiS as afunction of the fraction s/^a of the total space filled
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