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LM3224 датащи(PDF) 13 Page - Texas Instruments |
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LM3224 датащи(HTML) 13 Page - Texas Instruments |
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13 / 27 page ![]() m1 # VINRDSON L (in V/s) n = 1+ 2mc m1 (no unit) Leff = L (D') 2 Z c (in rad/s) 2fs nD' # ADC(DB) = 20log10 {[(ZcLeff)// RL]//RL} (in dB) RFB1 + RFB2 RFB2 ( ) gmROD' RDSON LM3224 www.ti.com SNVS277C – DECEMBER 2004 – REVISED MARCH 2013 The inductor ripple current is important for a few reasons. One reason is because the peak switch current will be the average inductor current (input current or ILOAD/D') plus ΔiL. As a side note, discontinuous operation occurs when the inductor current falls to zero during a switching cycle, or ΔiL is greater than the average inductor current. Therefore, continuous conduction mode occurs when ΔiL is less than the average inductor current. Care must be taken to make sure that the switch will not reach its current limit during normal operation. The inductor must also be sized accordingly. It should have a saturation current rating higher than the peak inductor current expected. The output voltage ripple is also affected by the total ripple current. The output diode for a boost regulator must be chosen correctly depending on the output voltage and the output current. The typical current waveform for the diode in continuous conduction mode is shown in Figure 22 (b). The diode must be rated for a reverse voltage equal to or greater than the output voltage used. The average current rating must be greater than the maximum load current expected, and the peak current rating must be greater than the peak inductor current. During short circuit testing, or if short circuit conditions are possible in the application, the diode current rating must exceed the switch current limit. Using Schottky diodes with lower forward voltage drop will decrease power dissipation and increase efficiency. DC GAIN AND OPEN-LOOP GAIN Since the control stage of the converter forms a complete feedback loop with the power components, it forms a closed-loop system that must be stabilized to avoid positive feedback and instability. A value for open-loop DC gain will be required, from which you can calculate, or place, poles and zeros to determine the crossover frequency and the phase margin. A high phase margin (greater than 45°) is desired for the best stability and transient response. For the purpose of stabilizing the LM3224, choosing a crossover point well below where the right half plane zero is located will ensure sufficient phase margin. To ensure a bandwidth of ½ or less of the frequency of the RHP zero, calculate the open-loop DC gain, ADC. After this value is known, you can calculate the crossover visually by placing a −20dB/decade slope at each pole, and a +20dB/decade slope for each zero. The point at which the gain plot crosses unity gain, or 0dB, is the crossover frequency. If the crossover frequency is less than ½ the RHP zero, the phase margin should be high enough for stability. The phase margin can also be improved by adding CC2 as discussed later in this section. The equation for ADC is given below with additional equations required for the calculation: (8) (9) (10) (11) mc ≊ 0.072fs (in V/s) (12) where • RL is the minimum load resistance • VIN is the minimum input voltage • gm is the error amplifier transconductance found in the Electrical Characteristics table • RDSON is the value chosen from the graph "NMOS RDSON vs. Input Voltage" in the Typical Performance Characteristics section (13) Copyright © 2004–2013, Texas Instruments Incorporated Submit Documentation Feedback 13 Product Folder Links: LM3224 |
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