Page 190 - Power Electronics Handbook
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182   Phase-controlled rectification and inversion

                            varying load power factor as the  firing angle is changed.  For  net
                            rectification this power factor is lagging, although for inversion it
                            changes to leading.
                        (iii)  The  mean  d.c.  load  voltage  decreases  as  the  firing  angle  (Y  is
                            increased, and beyond 90" delay the voltage goes negative, reaching a
                            peak negative value at 180'.  Clearly, for a.c. to d.c. rectifier systems
                            the negative voltage period is undesirable.
                        (iv)  The value of the d.c. ripple voltage also increases as the firing angle is
                            increased, up  to  90" delay.  Beyond  this  point  the  ripple  in  the
                            negative voltage decreases as (Y is increased to 180'.
                        (v)  The  period  for  which  a  thyristor  is  reverse  biased  reduces
                            progressively as the delay angle increases to 180". A thyristor must, of
                            course, be reverse biased for greater than its turn-off time in order to
                            be successfully commutated. Therefore the maximum delay angle can
                            never be raised to 180" and for practical systems it is normally limited
                            to  about  165" on  SoHz  systems.  If  a  thyristor is  not  successfully
                            commutated  it  will  commence  conduction  the  instant  its  anode
                            voltage goes positive and so provide a complete half cycle of power to
                            the load. There will therefore be an abrupt change in the converter
                            operating mode from almost full inversion to full rectification.
                          Push-pull  converter circuits are popularly used  in  applications which
                        require an input transformer either for isolation purposes or for effective
                        phase number increase. As  will be  seen later, the larger the number of
                        input phases, the lower the d.c. voltage ripple and the higher the power
                        which the converter can handle. However, when an input transformer is
                        not  essential a bridge  system is often more economical, a single-phase
                        bridge being shown in Figure 9.4.  The operation of  this bridge can be


                                                6
                          TH1
                       A-
                        0-
                         TH3          TH4
                       Figwe 9.4 Bridge-type two-pulse bi-directional converter

                       followed by the waveforms of  Figure 9.3, where THI, TJ&  and TH2, TH,
                       conduct  in  pairs.  There  are  three  points  of  difference  between  the
                       push-pull  and bridge converters, as follows.
                       (i)  In a bridge system each thyristor must be rated to block the peak
                            voltage across the  a.c.  inputs of  the  converter, so  the  peak load
                            voltage and peak thyristor voltage are equal, whereas for a push-pull
                            system it was seen that the thyristors must be rated for at least twice
                            the peak load voltage.
                       (ii)   A push-pull  converter uses two devices compared to the four used
                            for a  bridge  system, but their voltage rating is now  doubled.  For
                            low-power systems the price of a thyristor is usually determined by its
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