Page 157 - Rashid, Power Electronics Handbook
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146                                                                                 Y.-S. Lee and M. Chow

               TABLE 10.3  Important design parameters of three-phase recti®er circuits with resistive load

                                                 Three-Phase Star Recti®er  Three-Phase Double-Star Recti®er  Three-Phase Bridge Recti®er
                                                                        With Inter-Phase Transformer
               Peak repetitive reverse voltage V RRM  2.092 V dc        1.06 V dc                   1.05 V dc
               Rms input voltage per transformer leg V s  0.855 V dc    0.855 V dc                  0.428 V dc
               Diode average current I FðAVÞ     0.333 I dc             0.167 I dc                  0.333 I dc
               Peak repetitive forward current I FRM  3.63 I FðAVÞ      3.15 I FðAVÞ                3.14 I FðAVÞ
               Diode rms current I FðRMSÞ        0.587 I dc             0.293 I dc                  0.579 I dc
                                                 1.76                   1.76                        1.74
               Form factor of diode current I FðRMSÞ =I FðAVÞ
               Recti®cation ratio                0.968                  0.998                       0.998
               Form factor                       1.0165                 1.0009                      1.0009
               Ripple factor                     0.182                  0.042                       0.042
               Transformer rating primary VA     1.23 P dc              1.06 P dc                   1.05 P dc
               Transformer rating secondary VA   1.51 P dc              1.49 P dc                   1.05 P dc
               Output ripple frequency f r       3 f i                  6 f i                       6 f i















                        FIGURE 10.9  Three-phase inter-star recti®er.

               Table 10.3). Furthermore, a star-connected primary winding
               with no neutral connection is equally permissible because the
               sum of all primary phase currents is zero at all times.
                                                                    FIGURE 10.10  Three-phase double-star recti®er with interphase trans-
                                                                    former.

               10.3.1.3 Three-Phase Double-Star Rectifier with
                        Interphase Transformer                      at all times. Therefore, a star primary winding with no neutral
               This circuit consists essentially of two three-phase star recti-  connection would be equally permissible.
               ®ers with their neutral points interconnected through an
               interphase transformer or reactor. The polarities of the corre-  10.3.2 Three-Phase Bridge Rectifiers
               sponding secondary windings in the two interconnected
               systems are reversed with respect to each other, so that the  Three-phase bridge recti®ers are commonly used for high-
               recti®er output voltage of one three-phase unit is at a mini-  power applications because they have the highest possible
               mum when the recti®er output voltage of the other unit is at a  transformer utilization factor for a three-phase system. The
               maximum as shown in Fig. 10.10. The interphase transformer  circuit of a three-phase bridge recti®er is shown in Fig. 10.12.
               causes the output voltage v to be the average of the recti®ed
                                      L
               voltages v and v as shown in Fig. 10.11. In addition, the
                        1
                              2
               ripple frequency of the output voltage is now six times that of
               the mains and, therefore, the component size of the ®lter (if
               there is any) becomes smaller. In a balanced circuit, the output
               currents of two three-phase units ¯owing in opposite direc-
               tions in the interphase transformer winding will produce no
               dc magnetization current. Similarly, the dc magnetization
               currents in the secondary windings of two three-phase units
               cancel each other out. By virtue of the symmetry of the  FIGURE 10.11  Voltage waveforms of the three-phase double-star recti-
               secondary circuits, the three primary currents add up to zero  ®er.
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