Protorit.blogspot.com Website Review


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Country: United States
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Latitude: 37.751
Longitude: -97.822




Summarized Content

POWER, ELECTRONIC SYSTEMS, APPLICATIONS AND RESOURCES ON ELECTRICAL AND ELECTRONIC PROJECT-THESIS. Wound rotor induction generators (WRIGs) are provided with three phase windings on the rotor and on the stator. They may be supplied with energy at both rotor and stator terminals. This is why they are called doubly fed induction generators (DFIGs) or double output induction generators (DOIGs). Both motoring and generating operation modes are feasible, provided the power electronics converter that supplies the rotor circuits via slip-rings and brushes is capable of handling power in both directions. As a generator, the WRIG provides constant (or controlled) voltage Vs and frequency f1 power through the stator, while the rotor is supplied through a static power converter at The rotor circuit may absorb or deliver electric power. As the number of poles of both stator and rotor windings is the same, at steady state, according to the frequency theorem, the speed ωm is as follows: FIGURE 1.1 Wound rotor induction generator (WRIG) main operation modes: (a) basic configuration, (b) subsynchronous generating (ωr < ω1), (c) supersynchronous generating (ωr > ω1), and (d) rotor output WRIG (brushless exciter). The sign is positive (+) in Equation 1.1 when the phase sequence in the rotor is the same as in the stator and ωm < ω1, that is, subsynchronous operation. The negative (−) sign in Equation 1.1 corresponds to an inverse phase sequence in the rotor when ωm > ω1, that is, supersynchronous operation. For constant frequency output, the rotor frequency ω2 has to be modified in step with the speed variation. This way, variable speed at constant frequency (and voltage) may be maintained by controlling the voltage, frequency, and phase sequence in the rotor circuit. It may be argued that the WRIG works as a synchronous generator (SG) with three-phase alternating current (AC) excitation at slip (rotor) frequency ω2 = ω1 − ωm. However, as ω1 ≠ ωm, the stator


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