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VIPER38HD 数据表(PDF) 21 Page - STMicroelectronics |
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VIPER38HD 数据表(HTML) 21 Page - STMicroelectronics |
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21 / 31 page ![]() DocID025703 Rev 2 21/31 VIPER38 Operation 31 When the feedback pin voltage reaches the threshold VFBlin, an internal current generator starts to charge the feedback capacitor (CFB) and when the feedback voltage reaches the VFBolp threshold, the converter is turned off and the automatic restart is activated. During startup, when the output voltage is still low, if the feedback network is not properly dimensioned, the feedback voltage could rise up to the overload threshold (VFBolp) generating the switching off of the IC itself. Taking into account that the feedback network also fixes the loop stability, two options can be considered for this network. The time from the overload detection (VFB = VFBlin) to the device shutdown (VFB = VFBolp) must be set by CFB (or CFB1) using the formula: Equation 5 In the option 1 shown in Figure 23: FB pin configuration (option 1), the capacitor CFB has a dual function: guaranteeing the loop compensation and fixing the overload delay time as calculated in Equation 5. Owing to the above considerations, the OLP delay time must be long enough to bypass the initial output voltage transient and check the overload condition only when the output voltage is in steady state. The output transient time depends on the value of the output capacitor and on the load. When the value of the CFB capacitor calculated for the loop stability is too low and cannot ensure enough OLP delay, an alternative compensation network can be used and it is shown in Figure 24: FB pin configuration (option 2). Using this alternative compensation network, two poles (fPFB, fPFB1) and one zero (fZFB) are introduced by the capacitors CFB and CFB1 and the resistor RFB1. The capacitor CFB introduces a pole (fPFB) at higher frequency than fZB and fPFB1. This pole is usually used to compensate the high-frequency zero due to the ESR (equivalent series resistor) of the output capacitance of the flyback converter. The mathematical expressions of these poles and zero frequency are: Equation 6 Equation 7 The RFB(DYN) is the dynamic resistance seen by the FB pin. T OLP delay – C FB V FBolp V FBlin – I FB2 ---------------------------------------- × = f ZFB 1 2 π C FB1 R FB1 ⋅⋅ ⋅ ----------------------------------------------- = f PFB R FB DYN () R FB1 + 2 π C FB R FB DYN () RFB1 ⋅ () ⋅⋅ ⋅ ------------------------------------------------------------------------------- = () ) DYN ( FB 1 FB 1 FB 1 PFB R R C 2 1 f + ⋅ ⋅ π ⋅ = |
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