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VIPER53EDIP-E 数据表(PDF) 16 Page - STMicroelectronics |
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VIPER53EDIP-E 数据表(HTML) 16 Page - STMicroelectronics |
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16 / 31 page ![]() Regulation Loop Stability VIPer53EDIP - E / VIPer53ESP - E 16/31 DocRev1 10 Regulation Loop Stability The complete converter open loop transfer function can be built from both power cell and the feedback network transfer functions. A theoretical example can be seen in Figure 11 on page 22 for a discontinuous mode flyback loaded by a simple resistor. A typical schematic corresponding to this situation can be seen on Figure 3 on page 8. The transfer function of the power cell is represented as G(s) in .Figure 11 on page 22 It exhibits a pole which depends on the output load and on the output capacitor value. As the load of a converter may change, two curves are shown for two different values of output resistance value, RL1 and RL2. A zero at higher frequency values then appears, due to the output capacitor ESR. Note: The overall transfer function does not depend on the input voltage because of the current mode control. A typical regulation loop is shown on Figure 3 on page 8 and has a fixed behavior represented by F(s) on Figure 11 on page 22. A double zero due to the R1-C1 network on the COMP pin and to the integrator built around the TL431 and R2-C2 is set at the same value as the maximum load RL2 pole. The total transfer function is shown as F(s). G(s) at the bottom of Figure 11 on page 22. For maximum load (plain line), the load pole begins exactly where the zeros of the COMP pin and the TL431 stop, and this results in a first order decreasing slope until it reaches the zero of the output capacitor ESR. The point where the complete transfer function has a unity gain is known as the regulation bandwidth and has a double interest: – The higher it is, the faster the reaction will be to an eventual load change, and the smaller the output voltage change will be. – The phase shift in the complete system at this point has to be less than 135° to ensure good stability. Generally, a first-order slope gives 90° of phase shift, and a second-order gives 180°. In Figure 3 on page 8, the unity gain is reached in a first order slope, so the stability is ensured. The dynamic load regulation is improved by increasing the regulation bandwidth, but some limitations have to be respected: 1. As the transfer function above zero due the ESR capacitor is not reliable (the ESR itself is not well specified, and other parasitic effects may take place), the bandwidth should always be lower than the minimum of FC and ESR zero 2. As the highest bandwidth is obtained with the highest output power (plain line with RL2 load in Figure 3, the above criteria will be checked for this condition and allows the value of R4 if R1 is set to a fixed value (e.g., (2.2k Ω). As the highest bandwidth is obtained with the highest output power (Plain line with RL2 load in Figure 3), the above criteria will be checked for this condition and allows to define the value of R4, if R1 is set fixed (2.2kΩ, for instance). The following formula can be derived: Go is the current transfer ratio of the optocoupler. R 4 P MA X P OUT2 --------------------- G O R 1 ⋅ F BW 2 R L2 C OUT ⋅⋅ -------------------------------------------------------- ⋅ = P OUT2 V OUT 2 R L2 ----------------- = with: P MA X 1 2 --- L P I LIM 2 F SW ⋅⋅ ⋅ = and: |
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