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AN2872 Arkusz danych(PDF) 7 Page - STMicroelectronics |
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AN2872 Arkusz danych(HTML) 7 Page - STMicroelectronics |
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7 / 23 page ![]() AN2872 Description Doc ID 15305 Rev 1 7/23 The regulator of the circuit measures the output voltage, compares it with the reference voltage and modifies the duration of the ON time to keep the output voltage constant. In cases where the inductor current is operating in the continuous mode (the current does not cross zero at full load) the duty cycle can be obtained using Equation 2. This formula follows from Equation 1. Another method to obtain Equation 2 is to consider the buck converter as a low pass filter (L1, C2), connected to a rectangular signal and that the low pass filter generates a mean value. Equation 2 3.1.2 Practical aspects of a buck converter dedicated for mains and 3-phase input The application of a mains or 3-phase buck converter using a simple monolithic device results in several special conditions. A few of the most important are described in the following paragraphs. The operation of a buck converter such as that of the diagram in Figure 2 requires an active high side switch. Therefore, the monolithic device (with integrated N-channel MOSFET) is also connected on the high side (between + of bulk capacitor and inductor). The GND of the controller connected to the source of the MOSFET refers to the high side of the inductor (see Figure 3). This wiring of circuit causes the feedback signal not to be directly sensed from the output due to the shift of the GND of output voltage and controller. Basically, there are two ways to move the information regarding the output voltage from the output to the controller. The first way is to apply an optocoupler between the output and the converter. The additional error amplifier and reference (typically TL431 or a simple Zener diode) must be assembled to drive the LED of the optocoupler. This method gives high precision of the output voltage level and low load regulation. However, it also increases the cost and space requirements. The second principle is to use a replica of the output voltage stored in the auxiliary capacitor during OFF time. The schematic in Figure 3 shows the principle connection of the components. The auxiliary capacitor C3 is charged during the OFF time from inductor L1 to the same voltage level as capacitor C2. It can be expected that the voltage drop over both capacitors (C2 and C3) must be equal. However, in real applications the voltages are not exactly the same. This difference is caused by the difference in the discharge current of capacitors, different capacitance and different voltage drop on diodes D1 and D2. An important effect of the variance of the voltage drop of C2 and C3 is the fact that only C2 is charged during ON time. Due to this behavior it is possible to see a theoretically unlimited increase in the output voltage at light or no load, because the energy delivered during the ON time is higher than the total energy required by the load. Therefore, an additional load (resistor) or voltage limiter (Zener diode) is required on the output to protect the output capacitor and the load against overvoltage at light load. δ V 2 V 1 ------ = |
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