Page 281 - Power Electronics Handbook
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D.C. to d.c. convener circuits   271

                   resonant paths. For zero loss the voltage would reach an infinite value. To
                   limit  this  voltage  boost  a  free-wheeling diode  is  sometimes  connected
                   across b. This means that when C has discharged to zero volts the energy
                   stored in   is dissipated in the free-wheel path and there is no build-up of
                   capacitor voltage. The price paid is loss of  efficiency.
                     Figure  12.9 shows a  modification to the circuit of  Figure  12.7 which
                   prevents  excessive commutation  capacitor voltage build-up,  resulting in
                   increased  device voltage  rating,  whilst  still maintaining high  efficiency.
                   Winding L3 is closely coupled to   and normally has a voltage induced in it
                   such that D1 is reverse biased. During the commutation interval, however,
                   when the voltage on   reverses, D1 will conduct, clamping   to VB and
                   resulting in an overshoot across L,  of a value given by equation (1 2.7) which
                   can  be  made  small. There is theoretically no commutation loss  since the
                   commutation energy stored in L2 is fed back to the supply by  L3.


                                                                              (12.7)


                   12.2.3.3 Voltage boosting
                   If  the commutation voltage is high, the commutation capacitor can have a
                   low  value  and  still  provide  the  same  turn-off  energy  required  for  the
                   thyristors.  For instance, in the chopper circuit of  Figure 12.4 if  tom  is the
                   turn-off  time  of  THI then,  to  commutate  a  peak  current  of  tL(pk),  the
                   capacitor size required is given by

                     C=   IL(pk) fOFF                                         (12.8)
                             vc
                     In  this  equation  V,  is  the  commutation  capacitor  voltage  prior  to
                   commutation and in the circuit of Figure 12.4 it can have a maximum value
                   of  VB. This equation shows that to commutate a current of  500A, with a
                   voltage across the commutation capacitor of  20V and using 20 ps turn-off
                   time thyristors, would require  a capacitor of  500pF, 20V rating.  If  the
                   value  of  V, is increased  by  a  factor of  10, by  some method  of  voltage
                   boosting, a commutation capacitor of 50 pF, 200 V will be needed, which is
                   smaller and cheaper. Another disadvantage of using high-valued capacitors
                   is that the resonant time of  C through L is increased. Suppose that this is
                   limited to 0.1 ms, to give sufficient output voltage control at high operating
                   frequencies. Then L must be 2 pH, which is impracticable, since normally
                   the  inductance  of  connecting  leads  would  be  greater  than  this  value.
                   Clearly,  a  voltage  system which  increased  V, and reduced  C would  be
                   advantageous.
                     Figure 12.10 shows a modification to Figure 12.4 where a series inductor
                   Ls is used to increase the commutation voltage. When TH, is conducting
                   suppose that the load current reaches a value of 1,.  Thyristor TH2 is fired
                   to turn the main thyristor off and capacitor C discharges at constant current
                  Z,,  assuming that the load inductance is sufficiently large to maintain the
                   current  at  this  value  during  the  short  capacitor  discharge  period.  C
                   recharges to Vs with plate b positive. Normally, if   were not present,
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