. The Bell System technical journal . esistivity is required. Thelower limit on s^ will be determined by internal loss mechanisms nottreated here. Experimentally, this lower bound is found to be approxi-mately oe-/isec. Reversal by Single Wall The switching time of a twistor when operating in a memory arrayunder coincident current conditions will depend upon the low^-driveswitching coefficient. Experimentally, it is observed that the low driveSy, is several times the high-drive value. In this section, following themethod of Williams, Shockley, and Kittel,^ flux reversal by the move-me
. The Bell System technical journal . esistivity is required. Thelower limit on s^ will be determined by internal loss mechanisms nottreated here. Experimentally, this lower bound is found to be approxi-mately oe-/isec. Reversal by Single Wall The switching time of a twistor when operating in a memory arrayunder coincident current conditions will depend upon the low^-driveswitching coefficient. Experimentally, it is observed that the low driveSy, is several times the high-drive value. In this section, following themethod of Williams, Shockley, and Kittel,^ flux reversal by the move-ment of a single wall will be treated. Only the circular flux case will beconsidered. The technique used to obtain Sw is identical to that used in except it is postulated that a single wall concentric to the wiremoves either from the wire surface inward, or from the wire axis result is independent of the direction in which the wall moves. As-sume the wall moves from r = 0 to r = ro , as indicated in Fig. 8. In-.
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Keywords: ., bookcentury1900, bookdecade1920, booksubjecttechnology, bookyear1
