Page 56 - Power Electronics Handbook
P. 56

The gate turn-off switch   49













                   Figure 1.27  Comparison between a conventional and an asymmetrical thyristor:
                   (a) conventional;  (b) asymmetrical

                   modest  gate  signal at  the  trigger  terminal since  the  regenerative gate
                   signals are derived from the load current.
                     All the thyristor structures demibed so far have been symmetrical, in
                   that the forward and reverse blocking capabilities are optimised. Often,
                   however, a thyristor is used in  series with  another thyristor or a diode
                   which can provide the reverse blocking voltage needed by the circuit. It is
                   then possible to use  an asymmetrical thyristor (or ASCR), as shown in
                   Figure  1.27,  where a highly doped layer has been  added near  the  anode
                   junction, which stops the extension of the electrical field. The ASCR has a
                   reduced forward voltage drop and lower turn-on time, and so lower losses,
                   but also a lower reverse blocking voltage capability, so it is usually used in
                   applications where it is connected in series with another rectifying device.


                   1.10 The gate turn-off switch
                   The gate turn-off switch (GTO) is similar in construction to a thyristor,
                   having four layers, with three terminals, anode, cathode and gate. It is
                   turned on by current flowing into the gate terminal, as for a conventional
                   thyristor, but it can be turned off by taking current out of the gate, that is,
                   with negative gate current. The operation of  the GTO can be explained
                   with  reference to  the  two-transistor analogy of  Figure  1.25(c). Here gate
                   current ZG is shown as flowing into terminal G2, but assuming that the two
                   transistors  are in  conduction, then  if  gate  current is  taken  out  of  this
                   terminal, it will divert all the base current away from the n-p-n  transistor,
                   turning it off. If  ZG is the value of this negative gate current, then turn-off
                   will occur if  it exceeds that given by  equation (1.18).

                                                                              (1.18)

                     Defining the turn-off gain $om of  the GTO by equation (1.19),  allows
                   equation (1.18)  to be rewritten as in equation (1.20).
                     BOFF  = -                                                (1.19)
                            IA
                            ZG
   51   52   53   54   55   56   57   58   59   60   61