Flyback converter
Unlike the ideal transformer, current does not flow simultaneously in both windings of the flyback transformer. Rather, the flyback transformer magnetizing inductance assumes the role of the inductor of the buck-boost converter.
The magnetizing current is switched between the
primary and secondary windings. When transistor Q1 conducts, diode D1 is
reverse-biased. The primary winding then functions as an inductor, connected to
the input source Vg. Energy is stored in the magnetic field of the flyback
transformer. When transistor Q1 turns off, the current ceases to flow in the
primary winding.
The magnetizing current, referred to the secondary
winding, now forward-biases diode D1. Energy stored in the magnetic field of
the flyback transformer is then transferred to the dc load. Application of the
principle of inductor volt-second balance to the transformer primary winding
leads to the following solution for the conversion ratio of the flyback
converter:
M(g) = V/Vg
Thus, the conversion ratio of the flyback converter
is similar to that of the buck-boost converter, but with an added factor of n.
The flyback converter has traditionally been used in the high-voltage power
supplies of televisions and computer monitors.
It also finds
widespread application in switching power supplies at the 50 W to 100 W power
range. This converter has the advantage of very low parts count. Multiple
outputs can be obtained using a minimum number of added elements: each
auxiliary output requires only an additional winding, diode, and capacitor.
However, in comparison with buck-derived transformer-isolated
converters such as the full bridge and forward circuits, the fly back converter
has the disadvantage of poor cross regulation.
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