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RM2CRTR6W–. The Bell System technical journal . ituation. With the very narrow limits specified for the operating frequency of themagnetron, it was essential that the anode pretuning be done very precisely.Here, considerable difficulty was encountered with a pretuning arrange-ment in which the indication of resonance depended on the equivalent linelength of the output circuit between the anode block and the detector in thewave guide. Variability in this electrical length caused the actual resonanceto vary over a considerably wider range than the required 9375 ± 30 mc/s.By use of a detector connected at
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RF2A79H04–3D Illustration Eu Flag with silver paragraph sign
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RM2CNCM12–. The Bell System technical journal . 1000 2000 3000 4000 5000 6000 H, APPLIED FIELD IN OERSTEDS 7000 Fig. 7 — Measurement of x-™ ^nd k versus applied static field for three differ-ent discs, cut from the same ferrite block. large to be measured. Knowledge of A(l/Q) is not sufficient to determineXm — k in the resonance region because here the correction termA(l/Q)+(/?i — i?2) (cf. ecjuation 26) becomes comparable to the termA(l/Q)-(/?i + Rl) and is needed to compensate for the anomalous peakof the A(l/Q) curve. The loss parameters Xm ± k assume values ofthe order of 10- below and above reso
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