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![Theory and calculation of alternating current phenomena . Fig. 145. the impedance of the generator. Hence, dividing the oppositeside of the parallelogram, JSiEo, in the same way, we have: OEi =El = Theory and calculation of alternating current phenomena . Fig. 145. the impedance of the generator. Hence, dividing the oppositeside of the parallelogram, JSiEo, in the same way, we have: OEi =El =](https://c8.alamy.com/comp/2AJD2YC/theory-and-calculation-of-alternating-current-phenomena-fig-145-the-impedance-of-the-generator-hence-dividing-the-oppositeside-of-the-parallelogram-jsieo-in-the-same-way-we-have-oei-=el-=-generated-emf-of-the-motor-oe2-=-ei-=-emf-at-motorterminals-or-at-end-of-line-oez-=-e3-=-emf-at-generatorterminals-or-at-beginning-of-line-oeo-=-eq-=-generated-emfof-generator-the-phase-relation-of-the-current-with-the-emfs-ei-eq-de-pends-upon-the-current-strength-and-the-emfs-ei-and-0-214-figs-146-to-148-show-several-such-diagrams-for-differentvalues-of-ei-but-the-sa-2AJD2YC.jpg)