. The Bell System technical journal . t 1 2 3 4 5 6 10 15 20 m= 1234 . . . . . . . . .9001 For any given mode in any given cavity, the values of S and M can becalculated from (17). In general, these values will not coincide with thosewhich have been plotted, but by the same token, they will lie among a groupof four combinations which have been plotted. Since the changes in dis-tribution are smooth, mental two-way interpolation will present no difficu
. The Bell System technical journal . t 1 2 3 4 5 6 10 15 20 m= 1234 . . . . . . . . .9001 For any given mode in any given cavity, the values of S and M can becalculated from (17). In general, these values will not coincide with thosewhich have been plotted, but by the same token, they will lie among a groupof four combinations which have been plotted. Since the changes in dis-tribution are smooth, mental two-way interpolation will present no difficulty. Acknowledgment The final plates depicting the current distributions are the result of theefforts of many individuals in plotting, spray tinting of the background,inking of the streamlines on celluloid overlay, and photographing. Specialmention must be made, however, of the contribution of Miss Florence , who carried out all the lengthy calculations of the tables heretoattached and of the necessary data for the
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Keywords: ., bookcentury1900, bookdecade1920, booksubjecttechnology, bookyear1
