Download The Flyback Converter - Lecture Notes | ECEN 4517 and more Study notes Electrical and Electronics Engineering in PDF only on Docsity! The Flyback Converter Lecture notes ECEN4517 ! Derivation of the flyback converter: a transformer-isolated version of the buck-boost converter ! Typical waveforms, and derivation of M(D) = V/Vg ! Flyback transformer design considerations ! Voltage clamp snubber Derivation of the flyback converter The flyback converter is based on the buck-boost converter. Its derivation is illustrated in Fig. 1. Figure 1(a) depicts the basic buck-boost converter, with the switch realized using a MOSFET and diode. In Fig. 1(b), the inductor winding is constructed using two wires, with a 1:1 turns ratio. The basic function of the inductor is unchanged, and the parallel windings are equivalent to a single winding constructed of larger wire. In Fig. 1(c), the connections between the two windings are broken. One winding is used while the transistor Q1 conducts, while the other winding is used when diode D1 conducts. The total current in the two windings is unchanged from the circuit of Fig. 1(b); however, the a) b) + – L – V + Vg Q1 D1 + – L – V + Vg Q1 D1 1:1 c) d) + – LM – V + Vg Q1 D1 1:1 + – LM + V – Vg Q1 D11:n C Fig. 1. Derivation of the flyback converter: (a) buck-boost converter, (b) inductor L is wound with two parallel wires, (c) inductor windings are isolated, leading to the flyback converter, (d) with a 1:n turns ratio and positive output. 2 current is now distributed between the windings differently. The magnetic fields inside the inductor in both cases are identical. Although the two-winding magnetic device is represented using the same symbol as the transformer, a more descriptive name is “two- winding inductor”. This device is sometimes also called a “flyback transformer”. Unlike the ideal transformer, current does not flow simultaneously in both windings of the flyback transformer. Figure 1(d) illustrates the usual configuration of the flyback converter. The MOSFET source is connected to the primary-side ground, simplifying the gate drive circuit. The transformer polarity marks are reversed, to obtain a positive output voltage. A 1:n turns ratio is introduced; this allows better converter optimization. Analysis of the flyback converter The behavior of most transformer-isolated converters can be adequately understood by modeling the physical transformer with a simple equivalent circuit consisting of an ideal transformer in parallel with the magnetizing inductance. The magnetizing inductance must then follow all of the usual rules for inductors; in particular, volt-second balance must hold when the circuit operates in steady-state. This implies that the average voltage applied across every winding of the transformer must be zero. Let us replace the transformer of Fig. 1(d) with the equivalent circuit described above. The circuit of Fig. 2(a) is then obtained. The magnetizing inductance LM functions in the same manner as inductor L of the original buck-boost converter of Fig. 1(a). When transistor Q1 conducts, energy from the dc source Vg is stored in LM. When diode D1 conducts, this stored energy is transferred to the load, with the inductor voltage and current scaled according to the 1:n turns ratio. a) + – LM + v – Vg Q1 D11:n C transformer model iig R iC+ vL – b) + – LM + v – Vg 1:n C transformer model iig R iC+ vL – c) + – + v – Vg 1:n C transformer model i R iC i/n – v/n + + vL – ig =0 Fig. 2. Flyback converter circuit, (a) with transformer equivalent circuit model, (b) during subinterval 1, (c) during subinterval 2. t Iyboack transformer design
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