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IW1707 датащи(PDF) 8 Page - Dialog Semiconductor |
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IW1707 датащи(HTML) 8 Page - Dialog Semiconductor |
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8 / 13 page ![]() iW1707 Low-Power Off-Line Digital Green-Mode PWM Controller Rev. 0.2 iW1707 Page 8 MaRch 8, 2012 depletion NFET or BJT turns on, and the V CC capacitor begins to charge up again towards the start-up threshold to initiate a new soft-start process. In applications where the active start-up is not needed, the start-up resistor can be directly connected to the V CC pin without using the active start-up device, and the ASU pin can be left unconnected. Refer to Figure 3.3 for the application circuit. 9.3 Understanding Primary Feedback Figure 9.2 illustrates a simplified flyback converter. When the switch Q1 conducts during t ON(t), the current ig(t) is directly drawn from rectified sinusoid v g(t). The energy Eg(t) is stored in the magnetizing inductance L M. The rectifying diode D1 is reverse biased and the load current I O is supplied by the secondary capacitor C O. When Q1 turns off, D1 conducts and the stored energy E g(t) is delivered to the output. + vin(t) TS(t) IO VO D1 Q1 N:1 VAUX CO vg(t) ig(t) + – iin(t) id(t) Figure 9.2: Simplified Flyback Converter In order to tightly regulate the output voltage, the information about the output voltage and load current need to be accurately sensed. In the DCM flyback converter, this information can be read via the auxiliary winding or the primary magnetizing inductance (L M). During the Q1 on-time, the load current is supplied from the output filter capacitor C O. The voltage across LM is vg(t), assuming the voltage dropped across Q1 is zero. The current in Q1 ramps up linearly at a rate of: ( ) ( ) gg M di t v t dt L = (9.1) At the end of on-time, the current has ramped up to: ( ) ( ) _ g ON g peak M vt t it L × = (9.2) This current represents a stored energy of: ( )2 _ 2 M g g peak L E it = × (9.3) When Q1, turns off at t O, ig(t) in LM forces a reversal of polarities on all windings. Ignoring the communication-time caused by the leakage inductance L K at the instant of turn-off t O, the primary current transfers to the secondary at a peak amplitude of: ( ) ( ) _ P d g peak S N i t i t N = × (9.4) Assuming the secondary winding is master, and the auxiliary winding is slave, VAUX 0V VAUX = -VIN x NAUX NP VAUX = VO x NAUX NS 1 2 Figure 9.3: Auxiliary Voltage Waveforms The auxiliary voltage is given by: ( ) V AUX AUX O S N VV N = +∆ (9.5) and reflects the output voltage as shown in Figure 9.3. The voltage at the load differs from the secondary voltage by a diode drop and IR losses. Thus, if the secondary voltage is always read at a constant secondary current, the difference between the output voltage and the secondary voltage will be a fixed ΔV. Furthermore, if the voltage can be read when the secondary current is small, ΔV will also be small. With the iW1707, ΔV can be ignored. The real-time waveform analyzer in the iW1707 reads this information cycle-by-cycle. The part then generates a feedback voltage V FB. The VFB signal precisely represents |
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