Page 241 - Fluid Power Engineering
P. 241

208   Chapter Te n


                            Synchronous generator
                               with wound rotor
                       Gear
                        box                                         Grid
                                                         Transformer
              Turbine                 =
                                        ~
                                     Rectifier
              FIGURE 10-6 Schematic of a grid-connected synchronous generator with
              wound rotor. Power factor control is achieved by controlling the DC excitation
              of the wound rotor through the rectifier.

              through a power converter (AC to DC and then back to AC) before
              delivering to the grid.

              Variable-Speed Permanent Magnet Synchronous Generators
              The inherent nature of wind energy demands variable speed gener-
              ators. The reason may be seen in the torque-rotor speed curves for
              different wind speeds. A constant-speed generator is able to capture
              energy most efficiently only for single wind speed. In Fig. 10-9 (see
              later), the constant-speed generator captures the maximum power
              only for wind speed of 6 m/s; at other wind speeds, this type of gener-
              ator does not operate at peak power. A variable speed turbine that can
              change rotor speed such that the turbine is operating at peak power
              for all wind speeds (below the rated wind speed) will yield higher en-
              ergy output. This is the motivation for the movement toward variable
              speed generators.
                 A special case of permanent magnet synchronous generator
              (PMSG) is discussed in which the speed of the rotor is variable. With
              p as the number of poles in the rotor, and rotor turning at speed of ω r ,
              the EMF generated in the stator is:
                                             ω r p
                                    E g = K pm                   (10-30)
                                              2
              where K pm is a constant that depends on the strength of the magnet,
              ω r is the speed of the generator, and p is the number of poles.
                 Circuit and power equations are the same as Eqs. (10-25) to (10-29).
              For a grid-connected synchronous generator, V T is known. However,
              for a variable-speed generator there is an intermediate variable fre-
              quency voltage (V g ) that is delivered to the rectifier.
                                  −E g + i g Z + V g = 0         (10-31)
              Voltage, power, and torque are given by: 2

                                     V g = E g cos δ             (10-32)
   236   237   238   239   240   241   242   243   244   245   246