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0066_Frame_C20  Page 42  Wednesday, January 9, 2002  5:49 PM










                                                                            R 1
                                                                   Y 0           B 0


                                                                    V
                                                                    DC
                                                                 B 1               Y 1


                                                                            R 0

                       FIGURE 20.70  Simple synchronous motor.

                                                        T max


                                                Torque
                                                          Working  Unstable
                                                          Region  Region



                                                             Load Angle (δ)

                       FIGURE 20.71  Torque characteristic for a synchronous motor.

                       of the currents.
                                                               60f
                                                   N s =  --------------------------------------------------  (20.26)
                                                        number of pole pairs
                       where N s  is the speed of the field in revolutions per minute and f is the frequency of the supply currents.
                         The mechanical construction is shown in Fig. 20.70. The rotor field is supplied from a dc source and
                       the stator coils are supplied with a three-phase current. The rotating magnetic field is induced by the
                       stator coils and the rotor, which may be likened to a permanent bar magnet, aligns itself to the rotating
                       flux produced in the stator. When a mechanical load is driven by the shaft, the field produced by the
                       rotor is pulled out of alignment with that produced by the stator. The angle of misalignment is called
                       the “load angle.” The characteristics of synchronous motors are normally presented in terms of torque
                       against load angle, as shown in Fig. 20.71.
                         The torque characteristic is basically sinusoidal with

                                                        T =  T max sin δ                        (20.27)

                       where T max  is the maximum rated torque and δ is the load angle.
                         It is evident from Eq. (20.27) that synchronous motors have no starting torque and the rotor must
                       be run up to synchronous speed by some alternative means. One method utilizes a series of short-
                       circuited copper bars inserted through the outer extremities of the salient poles. The rotating magnetic
                       flux induces currents in these “grids” and the machine accelerates as if it were a cage-type induction
                       motor, see following section. A second method uses a wound rotor similar to a slip-ring induction motor.
                       The machine is run up to speed as an induction motor and is then pulled into synchronism to operate
                       as a synchronous motor.
                         The advantages of the synchronous motor are the ease with which the power factor can be controlled
                       and the constant rotational speed of the machine, irrespective of the applied load. Synchronous motors,



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