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AN2644 bảng dữ liệu(PDF) 36 Page - STMicroelectronics |
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AN2644 bảng dữ liệu(HTML) 36 Page - STMicroelectronics |
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36 / 64 page ![]() The LLC resonant half-bridge converter AN2644 36/64 Remarks 1. In the below-resonance capacitive mode operation, since current is continuously flowing on the secondary side, this is a CCM mode (as already stated, it corresponds to the CCMB mode defined in [3]. 2. The physical reason of this CCMB operation is, as previously pointed out, the large voltage developed across the resonant capacitor. A large energy level must be circulating in the tank circuit and this is consistent with R<Rcrit condition in order for the capacitive mode to take place. Capacitive operating mode is then likely to occur under heavy load, overload or short circuit conditions and appropriate countermeasures must be taken to handle this. 3. Note that in all the inductive modes the absolute value of the switched currents (i.e. the current IR when either power MOSFET is switched off) is always greater than (in CCM mode above resonance) or equal to (in all DCM modes) the current I(Lp). In the capacitive mode, instead, the absolute value of the switched currents is lower than that in Lp. This consideration is useful when analyzing the transitions of the node HB. 4. Unlike the other modes, in capacitive mode the secondary rectifiers D1 and D2 start conducting during the conduction period of Q2 and Q1, respectively. The initial current is zero and its di/dt is low, thus they have a soft turn-on. Also in this case the voltage across the secondary rectifiers reverses as a result of their currents going to zero. Then, ZCS is maintained even under these conditions and it is possible to conclude that the secondary rectifiers are soft-switched at both turn-on and turn-off under all operating conditions and that this property is inherent in the topology. In fact no assumption has been made about the tank circuit's parameters. Figure 23. No-load operation (cutoff): main waveforms I(D2) = D2 current V(D2) = D2 anode voltage I(Q2) = Q2 current I(Lp) = Lp (magnetizing) current Vc = Resonant capacitor voltage LVG = Q2 gate I(D1) = D1 current V(D1) = D1 anode voltage I(Q1) = Q1 current IR = Tank circuit’s current VHB = Node HB voltage HVG= Q1 gate t 0 t 1 t 2 t 4 t 5 t 3 Q1 OFF Q2 ON Q1 ON Q2 OFF t 6 Q1 ON Q2 OFF I(D2) = D2 current V(D2) = D2 anode voltage I(Q2) = Q2 current I(Lp) = Lp (magnetizing) current Vc = Resonant capacitor voltage LVG = Q2 gate I(D1) = D1 current V(D1) = D1 anode voltage I(Q1) = Q1 current IR = Tank circuit’s current VHB = Node HB voltage HVG= Q1 gate I(D2) = D2 current V(D2) = D2 anode voltage I(Q2) = Q2 current I(Lp) = Lp (magnetizing) current Vc = Resonant capacitor voltage LVG = Q2 gate I(D1) = D1 current V(D1) = D1 anode voltage I(Q1) = Q1 current IR = Tank circuit’s current VHB = Node HB voltage HVG= Q1 gate t 0 t 0 t 1 t 1 t 2 t 2 t 4 t 4 t 5 t 5 t 3 t 3 Q1 OFF Q2 ON Q1 ON Q2 OFF t 6 t 6 Q1 ON Q2 OFF |
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