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Chapter 17: Synchbonizino Aiitebkatobs

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1897
Section IDtheory-calculation-alternating-current-phenomena-1897-chapter-17
Locationlines 18829-19345
Statuscandidate
Word Count1654
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CHAPTER XVII. SYNCHBONIZINO AIiTEBKATOBS. 168. 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 In consequence thereof, if the driving power of one of sev- eral parallel-operating generators is withdrawn, this gene- rator will keep revolving in synchronism as a synchronous motor ; and the power with which it tends to remain in synchronism is the maximum power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. 169. 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. 169. 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 ...
... he voltage at the common bus bars be assumed Fig, 121. as zero line, or real axis of coordinates of the complex method ; and let — 252 AL TERN A TING-CURRENT PHENOMENA, [§ 1 74 e = difference of potential at the common bus bars of the two alternators, Z ^= r — jx = impedance of external circuit, K=s^»--|-y^ = admittance of external circuit; hence, the current in external circuit is /- —JX Let £i = fi —/<?/ = ^a (cos wj — jsm wi) = induced E.M.F. of first machine ; £^ = <f2 — yVj' = a^ (cos «2 — y sin wa) =*: induced E.M.F. of sec- ond m ...
... d, the one engine will pull, while the other is near the dead-point, and conversely. Consequently, alter- nately the one alternator will tend to speed up and the other slow down, then the other speed up and the first slow down. This effect, if not taken care of by fly-wheel capacity, causes a "hunting" or pumping action; that is, a fluctuation of the lights with the period of the engine revo- lution, due to the alternating transfer of the load from one engine to the other, which may even become so excessive as to throw the machines out of step. This dif ...
CHAPTER XVII. SYNCHBONIZINO AIiTEBKATOBS. 168. 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 ...
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  • Radiation / light: Compare the chapter’s radiation vocabulary with modern electromagnetic radiation, spectral frequency, wavelength, absorption, and illumination engineering.
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