Page 376 - Power Electronics Handbook
P. 376

366   Power semiconductor circuit applications









                       (a)                               (b)
                        Figure 14.14 The switching action of a commutator


                       anticlockwise direction. The function of  the commutator is to switch the
                       rotor poles,  by  reversing coil current,  as shown in Figure 14.14, and so
                       maintain unidirectional motion.
                         In Figure  14.13 if  brushes A and B were connected to a load and the
                       armature rotated in a clockwise direction, by an external mechanical force,
                       an e.m.f. would be induced in coil sides a and b, forcing current down side
                       b and up side a. The commutator ensures that this current is unidirectional
                       in the load and the machine is now a d.c. generator.
                         During motor action, when the rotor revolves, the changing flux induces
                       in it a voltage which will produce poles to oppose the stator flux, this being
                       referred to as the motor back e.m.f. This voltage is a function of the motor
                       speed and the strength of the field flux, being in effect secondary generator
                       action in a motor.
                         The function of  the commutator must  be clearly noted.  It senses the
                       rotor position, by virtue of its construction, and switches the rotor current,
                       at the appropriate instant, to ensure that torque is unidirectional in a motor
                       and that the generator output is d.c.
                         Figure  14.15 illustrates an elementary a.c.  motor,  which differs from
                       Figure 14.13 in that the commutator and brushes are removed and the ends
                       of  the  rotor  short-circuited.  Assume  magnetising  current  to  flow  and
                       produce field poles as illustrated. Now if the poles were caused to rotate
                       they would induce a current in the rotor coil, this current, by Lenz's law,
                       opposing the rotating stator field. Figure 14.15 shows two positions of  the
                       stator field, the rotor being assumed at a standstill, and illustrates that the

                             Pole
                           f rotation               Power current

                                                                           b
                                                                   (3' ''9
                                                                          R
                                                                         '
                                                                     X

                                                                    a   Torque


                                                                              Pole
                                                                              rotation
                       Figon 14.15 Induced rotor polarity during rotation of a stator field
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