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LM2716 Datasheet(PDF) 13 Page - National Semiconductor (TI) |
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LM2716 Datasheet(HTML) 13 Page - National Semiconductor (TI) |
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13 / 17 page ![]() Boost Operation (Continued) Resistance, denoted R ESR) capacitors be used such as ceramic, polymer electrolytic, or low ESR tantalum. Higher ESR capacitors may be used but will require more compen- sation which will be explained later on in the section. The ESR is also important because it determines the peak to peak output voltage ripple according to the approximate equation: ∆V OUT ) 2 ∆i LRESR (in Volts) A minimum value of 10µF is recommended and may be increased to a larger value. After choosing the output capaci- tor you can determine a pole-zero pair introduced into the control loop by the following equations: Where R L is the minimum load resistance corresponding to the maximum load current. The zero created by the ESR of the output capacitor is generally very high frequency if the ESR is small. If low ESR capacitors are used it can be neglected. If higher ESR capacitors are used see the High Output Capacitor ESR Compensation section. RIGHT HALF PLANE ZERO A current mode control boost regulator has an inherent right half plane zero (RHP zero). This zero has the effect of a zero in the gain plot, causing an imposed +20dB/decade on the rolloff, but has the effect of a pole in the phase, subtracting another 90˚ in the phase plot. This can cause undesirable effects if the control loop is influenced by this zero. To ensure the RHP zero does not cause instability issues, the control loop should be designed to have a bandwidth of less than 1⁄2 the frequency of the RHP zero. This zero occurs at a fre- quency of: where I LOAD is the maximum load current. SELECTING THE COMPENSATION COMPONENTS The first step in selecting the compensation components R C2 and CC2 is to set a dominant low frequency pole in the control loop. Simply choose values for R C2 and CC2 within the ranges given in the Introduction to Compensation section to set this pole in the area of 10Hz to 500Hz. The frequency of the pole created is determined by the equation: where R O is the output impedance of the error amplifier, approximately 850k Ω. Since R C2 is generally much less than R O, it does not have much effect on the above equation and can be neglected until a value is chosen to set the zero f ZC. f ZC is created to cancel out the pole created by the output capacitor, f P1. The output capacitor pole will shift with differ- ent load currents as shown by the equation, so setting the zero is not exact. Determine the range of f P1 over the ex- pected loads and then set the zero f ZC to a point approxi- mately in the middle. The frequency of this zero is deter- mined by: Now R C2 can be chosen with the selected value for CC2. Check to make sure that the pole f PC is still in the 10Hz to 500Hz range, change each value slightly if needed to ensure both component values are in the recommended range. After checking the design at the end of this section, these values can be changed a little more to optimize performance if desired. This is best done in the lab on a bench, checking the load step response with different values until the ringing and overshoot on the output voltage at the edge of the load steps is minimal. This should produce a stable, high performance circuit. For improved transient response, higher values of R C2 should be chosen. This will improve the overall band- width which makes the regulator respond more quickly to transients. If more detail is required, or the most optimal performance is desired, refer to a more in depth discussion of compensating current mode DC/DC switching regulators. HIGH OUTPUT CAPACITOR ESR COMPENSATION When using an output capacitor with a high ESR value, or just to improve the overall phase margin of the control loop, another pole may be introduced to cancel the zero created by the ESR. This is accomplished by adding another capaci- tor, C C4, directly from the compensation pin VC2 to ground, in parallel with the series combination of R C2 and CC2. The pole should be placed at the same frequency as f Z1, the ESR zero. The equation for this pole follows: To ensure this equation is valid, and that C C4 can be used without negatively impacting the effects of R C2 and CC2,fPC4 must be greater than 10f ZC. CHECKING THE DESIGN The final step is to check the design. This is to ensure a bandwidth of 1⁄2 or less of the frequency of the RHP zero. This is done by calculating the open-loop DC gain, A DC. 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 1⁄2 the RHP zero, the phase margin should be high enough for stability. The phase mar- gin can also be improved by adding C C4 as discussed earlier in the section. The equation for A DC is given below with additional equations required for the calculation: www.national.com 13 |
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