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L6599AD Datasheet(PDF) 21 Page - STMicroelectronics |
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L6599AD Datasheet(HTML) 21 Page - STMicroelectronics |
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21 / 35 page ![]() L6599A Application information Doc ID 15308 Rev 7 21/35 7.3 Soft-start Generally speaking, the purpose of soft-start is to progressively increase converter power capability when it is started up, so as to avoid excessive inrush current. In resonant converters the deliverable power depends inversely on frequency, soft-start is then done by sweeping the operating frequency from an initial high value until the control loop takes over. With the L6599A converter, soft-startup is simply realized with the addition of an R-C series circuit from pin 4 (RFmin) to ground (see Figure 27, left). Initially, the capacitor CSS is totally discharged, so that the series resistor RSS is effectively in parallel to RFmin and the resulting initial frequency is determined by RSS and RFmin only, since the optocoupler phototransistor is cut off (as long as the output voltage is not too far away from the regulated value): Equation 4 The CSS capacitor is progressively charged until its voltage reaches the reference voltage (2 V) and, consequently, the current through RSS goes to zero. This conventionally is imposed 5 times by selecting the constants RSS·CSS. Before reaching 2 V on Css, the output voltage should be already close to the regulated value and the feedback loop already taken over, so that it is the optocoupler phototransistor to determine the operating frequency from that moment onwards. During this frequency sweep phase the operating frequency decays following the exponential charge of CSS, that is, initially it changes relatively quickly but the rate of change gets slower and slower. This counteracts the non-linear frequency dependence of the tank circuit that makes the converter power capability change little as frequency is away from resonance and change very quickly as frequency approaches resonance frequency (see Figure 27, right). Figure 27. Soft-start circuit (left) and power vs. frequency curve in a resonant half bridge (right) As a result, the average input current smoothly increases, without the peaking that occurs with linear frequency sweep, and the output voltage reaches the regulated value with almost no overshoot. () SS min start R // RF CF 3 1 f ⋅ ⋅ = |
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