Page 271 - Power Electronics Handbook
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Chapter 12
                   D.C. to d.c. converters
















                   12.1 Introduction
                   To regulate the power between a d.c. source and a d.c.  load both linear
                   and  switching techniques can be  used.  Linear  regulators are  simpler in
                   design and provide a smoother output with less RFI generation, but they
                   dissipate much more power within the regulator. Therefore for high-power
                   applications switching regulators are almost invariably used.
                     The basic switching d.c. to d.c. regulator was introduced in Chapter 6,
                   and it was shown there that  both step-down and step-up controllers are
                   available. The step-down converter is the one most frequently used and
                   this is described in the next section, step-up converters being introduced in
                   Section 12.5.
                     Figure  12.1  shows  an  elementary  transistor  stepdown  converter
                   (chopper) which is similar to the basic circuit illustrated earlier in Figure
                   6.5 except that a power transistor is used as the switch element and an L-C
                   filter section is included to smooth the load voltage, as would normally be
                   required for a power supply application. Figure 12.1 also shows the circuit
                   waveforms and,  as  described with  reference  to  Figure  6.6,  the  output
                   voltage can be controlled by varying the frequency or the mark-space ratio
                   of  the conducting transistor switch. The mean output voltage across the
                   load is given by equation (12.1) where tc is the closed time of the switch and
                   to is its open time.

                                                                              (12.1)

                     When  the  transistor  switch is conducting, the  load  current  builds up
                   through the device. When the transistor turns off the load current switches
                   to the  free-wheeling diode  D1 and  the  current  slowly decays, until  the
                   transistor is turned on again at the start of  the next cycle.
                     The chopping frequency used must be high, to minimise the load ripple.
                   For example, the filter attenuation factor is given by  equation (1 2.2) where
                   Zi, is the impedance of the inductor L, and Zc, is the impedance of capacitor
                   Cl.
                          2,  + 2,
                     t=                                                       (12.2)
                             2,
                                                                                 26 I
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