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AN2025 Datasheet(PDF) 4 Page - STMicroelectronics |
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AN2025 Datasheet(HTML) 4 Page - STMicroelectronics |
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4 / 11 page ![]() AN2025 - APPLICATION NOTE 4/11 The first phase corresponds to the charging of the junction capacitance of the diode, Cj. The voltage across the diode VD decreases until it reaches the clamping voltage of the diode -VClamp (see figure 7). As was explained above, when the total current is equal to IPEAK, VD is equal to -VS. Once the current has reached IPEAK, it then increases to reach the value I1 corresponding to VD = -VClamp (see figure 7). Phase 2: t ∈ [t1, t2] At t = t1: iT = I1 vD = VClamp During this phase, the diode works in the ava- lanche region. Consequently, the voltage across the diode is equivalent to a voltage generator equal to VClamp. The total current increases linearly with a slope equal to: (see figure 7) After t2, the voltage across the diode increases towards -VS (see figure 7). These considerations show that: I1 < IPEAK III.2.3. Estimation of the maximum avalanche peak power: PPEAK_AV The figure 8 shows in blue color the total current IT (diode + snubber) and in black line the real avalanche current waveforms during the switching-off of the diode. Figure 8: Total current and avalanche current waveforms when the diode works in the avalanche area di T dt -------- VClampVs L F ---------------------------- = IPEAK I1 IAR tp < 1µs t2 iAVALANCHE iAVALANCHE VClamp RS CS iT iT t1 t I Phase2 Phase2 diT dt = V-V L Clamp S F RS VClamp iAVALANCHE CS LF iT VS |
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