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Chapter 23: Synchronizing Alternators

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1916
Section IDtheory-calculation-alternating-current-phenomena-chapter-23
Locationlines 25135-25681
Statuscandidate
Word Count1789
Equation Candidates In Section0
Figure Candidates In Section2
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CHAPTER XXIII SYNCHRONIZING ALTERNATORS 203. All alternators, when brought to synchronism with each other, operate in parallel more or less satisfactorily. This is due to the reversibility of the alternating-current machine; that is, its ability to operate as synchronous motor. In consequence thereof, if the driving power of one of several parallel-operating generators is withdrawn, this generator will keep revolving in synchronism as a synchronous motor; and the power with which it tends to' remain in synchronism is the maximum power which it can furnish as synchronous motor under the conditions of running, 204. The principal and foremost condition of parallel opera- tion of alternators is equality of frequency; that is, the trans- mission of power from the prime movers to the alternators must be such as to allow them to run at the same
... a synchronous motor; and the power with which it tends to' remain in synchronism is the maximum power which it can furnish as synchronous motor under the conditions of running, 204. The principal and foremost condition of parallel opera- tion of alternators is equality of frequency; that is, the trans- mission of power from the prime movers to the alternators must be such as to allow them to run at the same frequency without slippage or excessive strains on the belts or transmission devices. Rigid mechanical connection of the alternators cannot be con ...
... own in Fig. 144, let the voltage at the common busbars be assumed as zero line, or real axis of coordinates of the complex representation; and let e = difference of potential at the common busbars of the two alternators; SYNCHRONIZING ALTERNATORS 295 Z = r -^ jx = impedance of the external circuit; Y = 9 ~ jb == admittance of the external circuit; hence, the current in the external circuit is e I = r -\-jx = e(g - jh). Let El = ei -\- je'i = ai(cos di + j sin di) = generated e.m.f. of first machine; E2 = 62 -{- je'i ^ a2(cos ...
CHAPTER XXIII SYNCHRONIZING ALTERNATORS 203. All alternators, when brought to synchronism with each other, operate in parallel more or less satisfactorily. This is due to the reversibility of the alternating-current machine; that is, its ability to operate as synchronous motor. In consequence thereof, if the driving power of one of several parallel-operating generators is ...
... ernators must be such as to allow them to run at the same frequency without slippage or excessive strains on the belts or transmission devices. Rigid mechanical connection of the alternators cannot be con- sidered as synchronizing, since it allows no flexibility or phase adjustment between the alternators, but makes them essentially one machine. If connected in parallel, a difference in the field- excitation, and thus the generated e.m.f. of the machines, may cause large cross-current, since it cannot be taken care of by phase adjustment of the ma ...
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theory-calculation-alternating-current-phenomena-fig-143mnrmnmnwv Fig. 143. allel; as, for instance, by the arrangement shown in Fig. 143,line 25260
theory-calculation-alternating-current-phenomena-fig-144nal admittance of the second machine. Fig. 144. Then, er + e’r = al^•line 25324
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