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AN2644 Datasheet(PDF) 12 Page - STMicroelectronics |
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AN2644 Datasheet(HTML) 12 Page - STMicroelectronics |
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12 / 64 page ![]() The LLC resonant half-bridge converter AN2644 12/64 Figure 7. Equivalent schematic of a transformer including parasitic capacitance 2.2 The switching mechanism Still another way of classifying resonant converters would include the LLC resonant half- bridge in the family of "resonant-transition" converters. This nomenclature refers to the fact that in this class of converters power switches are driven in such a way that a resonant tank circuit is stimulated to create a zero-voltage condition for them to turn-on. To understand how this can be achieved in the LLC half-bridge, it is instructive to consider the circuits illustrated in Figure 8 where the switches Q1 and Q2 that generate the square wave input voltage to the resonant tank are power MOSFETs. Their body diodes DQ1, DQ2 are pointed out because they play an important role. In circuit a), the drain-to-source parasitic capacitances Coss1, Coss2 are pointed out as well. In fact, as far as voltage changes of the node HB are concerned, the parasitic capacitances Cgd and Cds are effectively in parallel, then Cgd+Cds=Coss has to be considered. Additionally, other contributors to the parasitic capacitance of the node HB (e.g. that formed between the case of the power MOSFETs and the heat sink, the intrawinding capacitance of the resonant inductor, etc.) are lumped together in the capacitor CStray. Note that Coss1, like Coss2, is connected between the node HB and a node having a fixed voltage (Vin for Coss1, ground for Coss2). Then, as far as voltage changes of the node HB are concerned, Coss1 is effectively connected in parallel to Coss2 and CStray. It is convenient to lump all of them together in a single capacitor CHB from the node HB to ground, as shown in the circuit b): Equation 4 which we will refer to in the following discussion. Note also that Coss1 and Coss2 are non- linear capacitors, i.e. their value is a function of the drain-to-source voltage. It is intended that their time-related equivalent value will be considered (see Appendix A). C HB C OSS1 C OSS2 C Stray ++ = |
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