. The Bell System technical journal . 100 50 0. 008 010 QW ai6 022 Q24 STANDING-WAVE RATIO PHASE IN CYCLES PER SECOND Fig. 50.—The normalized load conductance, the characteristic admittance of the resona-tor and the normalized electronic tuning range to half power plotted vs standing waveratio phase for a particular case involving a short misterminated line. The electronictuning for a matched line is shown as a heav\ horizontal line in the |ilot of (Aw/coo)! . phases. We can do this by obtaining the conductance and Ml from and using Fig. 15 to btain

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. The Bell System technical journal . 100 50 0. 008 010 QW ai6 022 Q24 STANDING-WAVE RATIO PHASE IN CYCLES PER SECOND Fig. 50.—The normalized load conductance, the characteristic admittance of the resona-tor and the normalized electronic tuning range to half power plotted vs standing waveratio phase for a particular case involving a short misterminated line. The electronictuning for a matched line is shown as a heav\ horizontal line in the |ilot of (Aw/coo)! . phases. We can do this by obtaining the conductance and Ml from and using Fig. 15 to btain (Aw/wo)j . In Fig. 50, the parametersGlIJc (the total characteristic admittance including the effect of the line),A, and, finally, (Aaj/wo)j have been plotted vs standing wave phase incycles. (Ac<j/ajo)j for a matched load is also shown. This example is ofcourse not tyi:)ical for all reflex oscillators: in some cases the electronic tuningmight be reduced or oscillation might stop entirely for the standing wavephases which produce high con

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Keywords: ., bookcentury1900, bookdecade1920, booksubjecttechnology, bookyear1