Page 244 - Power Electronics Handbook
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234   Direct a.c. frequency converters
                       Figure 10.14(a) shows that the circuit is essentially the usual arrangement
                       of a cycloconverter with the addition of an induction regulator, which is fed
                       from the three-phase supply, in series with the load. The output voltage
                       from the six-pulse converter is as illustrated in Figure 10.13(b) and to this is
                       added the  induction  regulator output,  so  as  to  give  the  resultant  load
                       voltage  of  the  form  shown  in  Figure  10.14(b).  Once  again,  the
                       approximation to a sine wave is very close.
                         Envelope cycloconverters are incapable of variable-frequency operation
                       and,  since  the  converter  thyristors  operate  like  diodes  during  any
                       half cycle, they cannot regenerate load current back to the supply. For this
                       to occur the firing angle on the thyristors would need to be delayed beyond
                       the start of a cycle, as in normal a.c. to d.c. converters. Therefore envelope
                       cycloconverters are incapable of handling inductive loads since they cannot
                       absorb its reactive power.  For  stable operation  it  is now  necessary  to
                       connect a capacitor in parallel across the load, to raise its overall power
                       factor. This disadvantage is not met with in phase-controlled converters,
                       where the firing angle can be shifted readily to meet any required direction
                       of  load current flow.


                       10.5 Phase-controlled cycloconverters
                       The  operation  of  a  phase-controlled  cycloconverter has  already  been
                       described with reference to a single-phase system, as in Figure 10.2. It is
                       seen that the load frequency can be controlled by the oscillation frequency
                       of  the firing point about 90". The load voltage amplitude is governed by the
                       extent of this oscillation about the mean firing point and the converter can
                       be readily switched from rectification to inversion by regulating the firing
                       angle. The same considerations apply for a three-phase converter, and the
                       load waveforms for the three phases of a typical six-pulse system are shown
                       in Figure 10.15.
                         Each  phase  of  the  cycloconverter is  made  up  of  basic  single-phase
                       converter blocks, as in Figure 10.3(a), and by adjusting the firing angles of
                       positive (t+)   and negative (a,,) systems such that ap+a,, is always equal to
                       180", the mean output voltage from the two groups is equal, so that there is



                                               Output from
                                               positive group


                                               Output from
                                               negative group

                                               Instantaneous voltage
                                               difference between
                                               positive and negative groups
                      -re   10.15 Instantaneous voltage difference between positive and negative groups of a
                      cycloconverter
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