The Buck converter
The forward
converter family which includes the push-pull and bridge types, are all based
on the buck converter, shown in Fig. 2. Its operation is straightforward. When
switch TR1 is turned on, the input voltage is applied to inductor L1 and power
is delivered to the output. Inductor current also builds up according to
Faraday’s law shown below:-
V = L dI/ dt
When the switch is turned off, the voltage across the inductor reverses and freewheel diode D1 becomes forward biased. This allows the energy stored in the inductor to be delivered to the output. This continuous current is then smoothed by output capacitor Co.
The LC
filter has an averaging effect on the applied pulsating input, producing a
smooth dc output voltage and current, with very small ripple components
superimposed. The average voltage/sec across the inductor over a complete
switching cycle must equal zero in the steady state. (The same applies to all
of the regulators that will be discussed.)
Neglecting
circuit losses, the average voltage at the input side of the inductor is VinD,
while Vo is the output side voltage. Thus, in the steady state, for the average
voltage across the inductor to be zero, the basic dc equation of the buck is
simply
Vo/ Vi = D
D is the
transistor switch duty cycle, defined as the conduction time divided by one
switching period, usually expressed in the form shown below:-
D = ton T ;
where T = ton + t off
Thus, the
buck is a stepdown type, where the output voltage is always lower than the
input. (Since D never reaches one.) Output voltage regulation is provided by
varying the duty cycle of the switch. The LC arrangement provides very
effective filtering of the inductor current. Hence, the buck and its
derivatives all have very low output ripple characteristics. The buck is
normally always operated in continuous mode ( inductor current never falls to
zero) where peak currents are lower, and the smoothing capacitor requirements
are smaller. There are no major control problems with the continuous mode buck.
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