Theory and calculation of alternating current phenomena . Fig. 145. the impedance of the generator. Hence, dividing the oppositeside of the parallelogram, EiEo, in the same way, we have: OEi =El = generated of the motor, OE2 = E2 = at motorterminals or at end of line, OE3 = Ez = at generatorterminals, or at beginning of line. OEo = Eq = generated generator. The phase relation of the current with the , Ei, Eq, de-pends upon the current strength and the , Ei and Eq. 214. Figs. 146 to 148 show several such diagrams for differentvalues of Ei, but the sam
Theory and calculation of alternating current phenomena . Fig. 145. the impedance of the generator. Hence, dividing the oppositeside of the parallelogram, EiEo, in the same way, we have: OEi =El = generated of the motor, OE2 = E2 = at motorterminals or at end of line, OE3 = Ez = at generatorterminals, or at beginning of line. OEo = Eq = generated generator. The phase relation of the current with the , Ei, Eq, de-pends upon the current strength and the , Ei and Eq. 214. Figs. 146 to 148 show several such diagrams for differentvalues of Ei, but the same value of I and £0. The motor diagrambeing given in drawn line, the generator diagram in dotted line. As seen, for small values of Ei the potential drops in the alter-nator and in the line. For the value of Ei = Eq the potentialrises in the generator, drops in the line, and rises again in the 304 ALTERNATING-CURRENT PHENOMENA. Fig. 146.
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