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STCMB1 数据表(PDF) 21 Page - STMicroelectronics |
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STCMB1 数据表(HTML) 21 Page - STMicroelectronics |
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21 / 59 page ![]() DocID028958 Rev 4 21/59 STCMB1 Application information 59 It is possible to prove that, when choosing: Equation 6 the average value of the inductor current in a switching cycle will be: Equation 7 (z) The block diagram and the relevant waveforms of the ECOT-controlled TM PFC are shown in Figure 9 and Figure 10. On the one hand, a negative threshold is placed on the current sensing pin ISEN_PFC (VISEN_PFC_Z = -25 mV, typ.): the on-time generator (ramp at pin TON) starts as the (negative) voltage on the pin ISEN_PFC goes below VISEN_PFC_Z. This is equivalent to having ILth = VISEN_PFC_Z/Rs, where Rs is the current sensing resistor. On the other hand, when the threshold VISEN_PFC_Z is crossed by the rising signal on the pin ISEN_PFC at the end of the off-time, an internal generator (Ios = 50 A typ.) is turned on, which sources the current out of the pin ISEN_PFC. This becomes a positive offset voltage on the pin itself, because of the external series resistor Ros (part of the RC filter of the pin). In this way, the crossing of the threshold VISEN_PFC_Z by the negative-going signal can be further delayed and the equivalent current threshold ILth set at: Equation 8 The value of the series resistor Ros can be adjusted to find the optimum ILth. As a starting point, one can select Ros based on the theoretical compensation condition: Equation 9 Note in Figure 10 the effect of this offset in the region VISEN_PFC > VISENPFC_Z (green portion of the inductor current waveform), compared to the unaffected waveform that would occur with Ros = 0 (black portion of the same waveform in the previous cycle). L C V I drain out Lth sin V L C T L I I I pk _ in drain C _ ON Lpk Lvy L 1 2 1 2 1 Rs R I V I OS OS Z PFC ISEN Lth _ _ OS Z PFC ISEN drain out OS I V L C V Rs R _ _ |
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