Page 286 - Power Electronics Handbook
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276   D.C. to d.c. converters

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                                L- tc -1
                                                        to-
                                               I                  I
                                I              I                  1
                                              Time
                        Fil[lue 12.15 Steady state load current waveform of a chopper
                        (iii)  The turn-on time of  the thyristors is short compared to the switching
                            period, so  the switching losses can be neglected.
                        (iv)  The d.c.  source impedance is negligible so  that energy can flow in
                            either direction through it without affecting the value of the voltage at
                            its terminals.
                        (v)  The load voltage VL is constant during a cycle of  operation.
                        (vi)  The load current is continuous although it will fluctuate during a duty
                            cycle, as in Figure 12.15.
                          With  these  assumptions  the  values  of  the  minimum    and
                        maximum (IL@k))  load current can be written down, from Figure 12.15, as
                        in equations (12.14) and (12.15).
                                   v
                                                 R
                          IL(min)  + - exp (-  ro)  [ 1 - exp (-   R  rc)]
                                      =
                          VBIR    VB
                                                                                  (12.14)





                                                                                  (12.15)
                          The mean  current  (IT(av)) through  the  thyristor  THl  and  the  mean
                        current      through the diode D1 can be found from Figure 12.15 as the
                        mean of  current il over time rc and of  i2 over time to, respectively. These
                        are as  in equations (12.16) and (12.17).

                         -=---      rC      LIR  p-exp(-:tc)]         [I-+]
                          zT(av)
                          V$R     t, + ro   tc + to
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