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IW3602 датащи(PDF) 11 Page - Dialog Semiconductor |
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IW3602 датащи(HTML) 11 Page - Dialog Semiconductor |
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11 / 19 page ![]() iW3602 AC/DC Digital Power Controller for Dimmable LED Drivers Rev. 1.0 iW3602 © 2015 Dialog Semiconductor (UK) Ltd. Datasheet 11 of 19 VCC VCC(ST) ENABLE Start-up Sequencing VIN Figure 9.7 : Start-up Sequencing Diagram 9.6 Understanding Primary Feedback Figure 9.8 illustrates a simplified flyback converter. When the switch Q1 conducts during tON(t), the current ig(t) is directly drawn from rectified vg(t). The energy Eg(t) is stored in the magnetizing inductance LM. The rectifying diode D1 is reversely biased and the load current IO is supplied by the secondary capacitor CO. When Q1 turns off, D1 conducts and the stored energy Eg(t) is delivered to the output. + vin(t) TS(t) IO VO VAUX N:1 D1 Q1 VAUX CO vg(t) ig(t) + – iin(t) id(t) Figure 9.8 : Simplified Flyback Converter In order to tightly regulate the output voltage, the information about the output voltage and load current must be accurately sensed. In the DCM flyback converter, this information can be read via the auxiliary winding or the primary magnetizing inductance (LM). During the Q1 on-time, the load current is supplied from the output filter capacitor CO. 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: () () g g M di t v t dt L = (9.6) At the end of on-time, the current ramps up to: _ () () g ON g peak M vt t i t L × = (9.7) This current represents a stored energy of: 2 _ () 2 M g g peak L E i t = × (9.8) When Q1 turns off, ig(t) in LM forces a reversal of polarities on all windings. Ignoring the communication-time caused by the leakage inductance LK at the instant of turn-off, the primary current transfers to the secondary at a peak amplitude of: _ () () P d g peak S N i t i t N = × (9.9) Assuming the secondary winding is master and the auxiliary winding is slave. VAUX 0V VAUX = -VIN x NAUX NP VAUX = VO x NAUX NS Figure 9.9 : Auxiliary Voltage Waveforms The auxiliary voltage is given by: () AUX AUX O S N V VV N = +∆ (9.10) and reflects the output voltage as shown in Figure 9.9. The voltage at the load differs from the secondary voltage by a diode drop and IR losses. The diode drop is a function of current, as are 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 is a fixed ΔV. If the voltage can be read when the secondary current is small, for example, at the knee of the auxiliary waveform (see Figure 9.9), then ΔV is also small. With the iW3602, ΔV can be ignored. The real-time waveform analyzer in the iW3602 reads the auxiliary waveform information cycle by cycle. The part then generates a feedback voltage VFB. The VFB signal precisely |
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