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Chapter 18: Synchronizing Alternators

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1900
Section IDtheory-calculation-alternating-current-phenomena-1900-chapter-18
Locationlines 17597-18052
Statuscandidate
Word Count1605
Equation Candidates In Section0
Figure Candidates In Section2
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CHAPTER XVIII. SYNCHRONIZING ALTERNATORS. 189. All alternators, when brought to synchronism with each other, will 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 In consequence thereof, if the driving power of one of sev- eral parallel-operating generators is withdrawn, this gene- rator will keep revolving in synchronism as a synchronous motor ; and the power with which it tends to remain in synchronism is the maximum power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. 190. The principal and foremost condition of parallel operation of alternators is equality of frequency ; that is, the transmission of power from the prime movers to the alternators must be such as to allow them to
... 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. 190. The principal and foremost condition of parallel operation of alternators is equality of frequency ; that is, the transmission 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 co ...
... let the voltage at the common bus bars be assumed Fig. 137. as zero line, or real axis of coordinates of the complex representation ; and let — SYNCHRONIZING ALTERNATORS. 315 e = difference of potential at the common bus bars of the two alternators, Z = r — jx = impedance of external circuit, Y = g -\-jb = admittance of external circuit ; hence, the current in external circuit is Let J?i = e-i — je\ = #2 (cos u>1 — j sin £>i) = induced E.M.F. of first machine ; £2 = e.2 — _/>•/ = a2 (cos w2 — j sin w2) = induced E.M.F. of sec- ond ma ...
CHAPTER XVIII. SYNCHRONIZING ALTERNATORS. 189. All alternators, when brought to synchronism with each other, will 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 sev- eral parallel-operating generat ...
... ternators 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 considered as synchronizing ; since it allows no flexibility or phase adjustment between the alternators, but makes them essentially one machine. If connected in parallel, a differ- ence in the field excitation, and thus the induced E.M.F. of the machines, must cause large cross-current ; since it cannot be taken care of by phase adjustment of the m ...
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theory-calculation-alternating-current-phenomena-1900-fig-136when operating in series, the coils of the transformer will Fig. 136. be without current. In this case, by interchange of power through the transformers, the series connection w…line 17731
theory-calculation-alternating-current-phenomena-1900-fig-137Fig. 137, let the voltage at the common bus bars be assumed Fig. 137. as zero line, or real axis of coordinates of the complexline 17741
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