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LM3477 数据表(PDF) 17 Page - National Semiconductor (TI) |
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LM3477 数据表(HTML) 17 Page - National Semiconductor (TI) |
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17 / 23 page ![]() Output Capacitor Selection (Continued) How the output voltage recovers after that initial excursion depends on how fast the inductor current falls and how large the output capacitance is. See Figure 10. The ESR and the capacitance of the output capacitor must be carefully chosen so that the output voltage overshoot is within the design’s specification V OS(MAX). If the total com- bined ESR of the output capacitors is not low enough, the initial output voltage excursion will violate the specification, see ∆V C1. If the ESR is low enough, but there is not enough output capacitance, the output voltage will travel outside the specification window due to the extra charge being dumped into the capacitor, see ∆V C2. The LM3477/A has output over voltage protection (OVP) which could trigger if the transient overshoot is high enough. If this happens, the controller will operate in hysteretic mode (see OVER VOLTAGE PROTEC- TION section) for a few cycles before the output voltage settles to its steady state. If this behavior is not desired, substitute V OVP (referred to the output) for VOS(MAX) (VOVP is found in the ELECTRICAL CHARACTERISTICS table) to find the minimum capacitance and maximum ESR of the output capacitor. Calculations for the Output Capacitor During a loading transient, the delta output voltage ∆V c has two changing components. One is the voltage difference across the ESR ( ∆V r), the other is the voltage difference caused by the gained charge ( ∆V q). This gives: ∆V c = ∆V r + ∆V q The design objective is to keep ∆V c lower than some maxi- mum overshoot (V OS(MAX)). VOS(MAX) is chosen based on the output load requirements. Both voltages ∆V r and ∆V qwill change with time. For ∆V r the equation is: where, R ESR = the output capacitor ESR ∆I OUT = the difference between the load current change I OUT(MAX) −IOUT(MIN) D MIN = Minimum duty cycle of device (0.165 typical) Evaluating this equation at t = 0 gives ∆V r(max). Substituting V OS(MAX) for ∆V r(MAX) and solving for RESR gives: The expression for ∆V q is: From Figure 11 it can be told that ∆V C will reach its peak value at some point in time and then decrease. The larger the output capacitance is, the earlier the peak will occur. To find the peak position, let the derivative of ∆V C go to zero, and the result is: The intention is to find the capacitance value that will yield, at t peak,a ∆V C that equals VOS(max). Substituting tpeak for t and equating ∆V C to VOS(max) gives the following solution for C OUT(MIN): The chosen output capacitance should not be less than 47µF, even if the solution for C OUT(MIN) is less than 47µF. Notice it is already assumed that the total ESR is no greater than R ESR(MAX), otherwise the term under the square root will be a negative number. Power MOSFET Selection The drive pin of LM3477/A must be connected to the gate of an external MOSFET. In a buck topology, the drain of the external N-Channel MOSFET is connected to the input and the source is connected to the inductor. The C B pin voltage provides the gate drive needed for an external N-Channel MOSFET. The gate drive voltage depends on the input volt- age (see TYPICAL PERFORMANCE CHARACTERISTICS). In most applications, a logic level MOSFET can be used. For very low input voltages, a sub-logic level MOSFET should be used. The selected MOSFET directly controls the efficiency. The critical parameters for selection of a MOSFET are: 1. Minimum threshold voltage, V TH(MIN) 2. On-resistance, R DS(ON) 200033B5 FIGURE 10. Output Voltage Overshoot Violation 200033B6 FIGURE 11. Output Voltage Overshoot Peak www.national.com 17 |
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