Page 414 - Power Electronics Handbook
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Electrical machine control   403

                    synchronous motor field winding, the a.c. output from the exciter being
                    rectified by rotating diodes D1 to D6 before being fed to the motor field.
                    During  run-up  switch  Sw  is  open and  the  field  windings  are  shorted
                    through  resistor  R, the  a.c.  exciter field being open circuit. When  the
                    machine nears synchronism centrifuge switch Sw closes, the exciter field
                    now becoming energised so that d.c. is applied to the synchronous motor
                    field and it locks onto the rotating stator field.








                   Synchronous
                     motor field









                                                                 Exciter field

                    Figure 14.55 A more efficient brushless synchronous motor than that in Figure  14.52


                      The above system suffers from two disadvantages: (1) it is not fully solid
                    state  since  switch  Sw  is  used;  (2)  resistor  R  is  connected  in  circuit
                    throughout run-up and synchronous operation, so that the motor efficiency
                    is  reduced.  Figure  14.55  shows  a  better arrangement. During  run-up  the
                    ax.  exciter  is  de-energised  as before.  An  alternating  voltage  is  now
                    induced in the synchronous motor field windings due to induction action,
                    and  it  can  be  very  large  and  destroy  the  field  diodes unless these  are
                    protected. Assuming end B to be positive to A, current will flow through
                    R1 and D1 to D6. TH3 is off since its gate is at a negative potential, equal to
                    two diode drops, with respect to its cathode. In the next half cycle, when
                    end A is positive to B, TH3 is reverse biased and still held off. The voltage
                    induced in the synchronous motor coil now rapidly builds up and when it
                    reaches the zener voltage of  diode D7 thyristor TH2 is turned on followed
                    closely by the breakover of diode D8 and the firing of TH1. The motor field
                    is now short-circuited through THl, TH2 and R1, which prevents damage
                    occumng to  the  diode bridge.  At  speeds close to synchronism the  a.c.
                    exciter is energised and current flows into the motor field and TH1 and
                    TH2 turn off when D1 and D4 first conduct. TH3 is forward biased and
                    turns on so that R1 is short-circuited and no longer plays any part in the
                    exciter operation. Zener diodes D7 and D8 are chosen to ensure that their
                    voltage is greater than the peak a.c. exciter voltage, so that TH1 and TH2
                    are held off.
                      With the above scheme the starting and synchronous performance of the
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