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SYNCHRONOUS GENERATORS

            12.24                     CHAPTER TWELVE

            the phasor diagram that the magnitude of E (  K  ) remains constant because I and
                                           A
                                                                       F
            remained unchanged, while E sin   (which is proportional to the output power as long as
                                 A
            V remains constant) has increased.
             T
              When the governor set point is increased, the no-load frequency and the output power
            of the generator increase. As the power increases, the magnitude of E remains constant
                                                               A
            while E sin   is increased further.
                 A
              If the output power of the generator is increased until it exceeds the power consumed by
            the load, the additional power generated flows back into the system (infinite bus). By def-
            inition, the infinite bus can consume or supply any amount of power while the frequency
            remains constant. Therefore, the additional power is consumed.
              Figure 12.29b illustrates the phasor diagram of the generator when the real power has
            been adjusted to the desired value. Notice that at this time, the generator has a slightly leading
            power factor. It is acting as a capacitor, requiring reactive power. The field current can be
            adjusted so the generator can supply reactive power. However, there are some constraints
            on the operation of the generator under these circumstances. The first constraint on the gen-
            erator is that when I is changing, the power must remain constant. The power given to the
                          F
            generator is P      .
                      in  app  m
              For a given governor setting, the prime mover of the generator has a fixed torque-speed
            characteristic. When the governor set point is changed, the curve moves. Since the generator
            is tied to the system (infinite bus), its speed cannot change. Therefore, since the governor
            set point and the generator’s speed have not changed, the power supplied by the generator
            must remain constant. Since the power supplied does not change when the field current is
            changing, then I cos 
 and E sin   (the distance proportional to the power in the phasor
                        A
                                 A
            diagram) cannot change.
              The flux   increases when the field current is increased. Therefore, E (  K  ) must
                                                                 A
            increase. If E increases while E sin   remains constant, then phasor E must slide along
                      A            A                            A
            the constant-power line shown in Fig. 12.30. Since  V is constant, the angle of  jX I
                                                                           S A
            changes as shown. Therefore, the angle and magnitude of I change.
                                                      A
              Notice that the distance proportional to Q (I sin 
) increases. This means that increasing
                                             A
            the field current in a synchronous generator operating in parallel with a power system
            (infinite bus) increases the reactive power output of the generator.
              In summary, when a generator is operating in parallel with a power system (infinite
            bus), the following are true:
            1. The power system connected to the generator controls the frequency and the terminal
              voltage.
            2. The real power supplied by the generator to the system is controlled by the governor
              set point.
            3. The reactive power supplied by the generator to the system is controlled by the field current.









              FIGURE 12.30  The effect of increasing the generator’s field current on the phasor diagram of
              the machine.



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