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AN2644 датащи(PDF) 25 Page - STMicroelectronics |
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AN2644 датащи(HTML) 25 Page - STMicroelectronics |
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25 / 64 page ![]() AN2644 The LLC resonant half-bridge converter 25/64 progressively turns into DCM operation as the output load is reduced and frequency is moved away from resonance. CCMA operation at heavy load Also in this case it is possible to identify six fundamentals subintervals. The relevant waveforms are illustrated in the timing diagram of Figure 17. Again, t0 is the instant when, with Q1 conducting and Q2 open, the tank current IR has a positive-going zero-crossing. a) t0 → t1. Q1 is ON and Q2 is OFF. This is the "energy taking" phase. It is identical to the corresponding phase seen in the operation at resonance with the only difference that at the end of this phase, at t=t1, it is still IR > I(Lp) and then I(D1)>0. b) t1 → t2. This is the deadtime during which both Q1 and Q2 are OFF. At t=t1 IR is greater than zero and provides the energy to let the node HB swing from Vin to 0, so that the body diode of Q2, DQ2, is injected. This allows IR to flow; IR slope changes to a higher negative value, so that it quickly approaches I(Lp), which is still increasing with the same slope. D1 conducts until IR equals I(Lp), and then becomes reverse biased, with a negative voltage equal to 2·Vout (plus the contribution from LL2, here not shown), I(Lp) slope changes sign and D2 starts conducting. This phase ends when Q2 is switched on at t=t2. Note that the time Tz needed for IR to hit I(Lp) is related to their values at t=t1 and their slopes after t=t1 and not to the duration of the deadtime TD. Here it is Tz = TD just by chance. Figure 17. Operation above resonance (f > fR1): main waveforms in CCMA operation at heavy load c) t2 → t3. Q1 is OFF and Q2 is ON. At t=t2 IR is diverted from DQ2 to the RDS(on) of Q2, so that no significant energy is lost during the turn-on transient. This phase, which ends when IR=0 at t=t3, is identical to the (t2, t3) phase of the operation at resonance. 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 Q1 OFF Q2 ON Q1 ON Q2 OFF t 0 t 0 t 1 t 1 t 2 t 2 t 4 t 4 t 5 t 5 t 3 t 3 t 6 t 6 Q1 ON Q2 OFF |
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