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Chapter 19: Induction Generators

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1916
Section IDtheory-calculation-alternating-current-phenomena-chapter-19
Locationlines 20446-21537
Statuscandidate
Word Count1524
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CHAPTER XIX INDUCTION GENERATORS 173. In the foregoing, the range of speed from 5 = 1, stand- still, to s = 0, synchronism, has been discussed. In this range the motor does mechanical work. It consumes mechanical power, that is, acts as generator or as brake outside of this range. For s > 1, backward driving. Pi becomes negative, repre- senting consumption of power, while D remains positive; hence, since the direction of rotation has changed, represents con- sumption of power also. All this power is consumed in the motor, w^hich thus acts as brake. For s < 0, or negative, Pi and D become negative, and the machine becomes an electric generator, converting mechanical into electric energy. The calculation of the induction generator at constant fre- quency, that is, at a speed increasing with
... its magnetic field. When operating in parallel with synchronous alternating cur- rent generators, the induction generator obviously takes its leading exciting current from the synchronous alternator, which thus carries a lagging wattless current. 175. To generate constant frequency, the speed of the in- duction generator must increase with the load. Inversely, when driven at constant speed, with increasing load on the induction generator, the frequency of the current generated thereby decreases. Thus, when calculating the characteristic curves of the ...
... calculating the characteristic curves of the constant-speed induction generator, due regard has to be taken of the decrease of frequency with increase of load, or what may be called the slip of frequency, s. Let, in an induction generator, Yo = go — jho = primary exciting admittance, Zo = To -\- jxo = primary self-inductive impedance, Zi = ri + jxi = secondary self-inductive impedance, reduced to primary, all these quantities being reduced to the frequency of synchronism with the speed of the machine, /. Let e = generated em.f., reduced to full fre ...
... uires that 237 238 ALTERNATING-CURRENT PHENOMENA the power-factor either of the external circuit or of the induction generator varies with the voltage, so as to permit the generator and the external circuit to adjust themselves to equality of power-factor. Beyond magnetic saturation the power-factor decreases; that is, the lead of current increases in the induction machine. Thus, when connected to an external circuit of constant power- factor the induction generator will either not generate at all, if its power-factor is lower than that of th ...
CHAPTER XIX INDUCTION GENERATORS 173. In the foregoing, the range of speed from 5 = 1, stand- still, to s = 0, synchronism, has been discussed. In this range the motor does mechanical work. It consumes mechanical power, that is, acts as generator or as brake outside of this range. For s > 1, backward driving. Pi becomes negative, repre- senting consumption of power, while D remains positive; hence, since the direction of rotation has changed, represents con- sumption of power also. All this power is co ...
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theory-calculation-alternating-current-phenomena-fig-125KX) Fig. 125. voltage will rise until by magnetic saturation in the induction generator its power-factor has fallen to equality with that ofline 20763
theory-calculation-alternating-current-phenomena-fig-126)00 Fig. 126. the efficiency.line 21111
theory-calculation-alternating-current-phenomena-fig-1270 Fig. 127. and the terminal voltage at the synchronous motor,line 21509
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