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ADP1821ARQZ-R7 数据表(PDF) 16 Page - Analog Devices |
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ADP1821ARQZ-R7 数据表(HTML) 16 Page - Analog Devices |
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16 / 24 page ![]() ADP1821 Rev. B | Page 16 of 24 If the zero produced by the ESR of the output capacitor pro- vides sufficient phase boost at crossover, Type II compensation is adequate. If the phase boost produced by the ESR of the output capacitor is not sufficient, another zero is added to the compen- sation network, and thus Type III is used. A general rule to determine the scheme whether the phase contribution of the ESR zero is greater than 70 degrees at crossover. In Figure 16, the location of the ESR zero corner frequency gives significantly different net phase at the crossover frequency. GAIN FREQUENCY PHASE LC FILTER BODE PLOT PHASE CONTRIBUTION AT CROSSOVER OF VARIOUS ESR ZERO CORNERS fSW fCO fESR3 fESR2 fESR1 0dB fLC –40dB/dec –20dB/dec 0° –90° –180° Φ1 Φ2 Φ3 Figure 16. LC Filter Bode Plot Using a linear approximation from Figure 16, the phase contri- bution of the ESR zero at crossover can be estimated by ESR CO ESR f f × × = 10 log 45 ϕ (25) If φESR ≥ 70, then Type II compensation is adequate. If φESR < 70, use Type III, as an additional zero is needed. The total phase of the system at crossover is the sum of the contributing elements, namely φT = φLC + φESR + φCOMP (26) where: φLC = −180. φESR is as calculated in Equation 25. φCOMP = −90 + φP + φZ (27) Note in the compensator phase expression shown in Equation 27, the −90 degree term is the phase contributed by the initial inte- grator pole. The φP is the additional phase contributed by the high frequency compensation poles placed above crossover, and φZ is the phase contributed by the compensation zeros placed below crossover. For the system to be stable at crossover, phase boost is required from the compensator. For stability, the total phase at crossover is designed to be equal to −120 degrees φT = φLC + φESR + φCOMP (28) −120 = −180 + φESR + −90 + φP + φZ (29) Define phase boost, φB, to be that portion of the phase at crossover contributed by the compensator’s higher order poles and zeros: φB = φP + φZ (30) φB = 150 − φESR (31) D. Venable, in his article “The K Factor: A New Mathematical Tool for Stability Analysis and Synthesis,” 1983, showed that an optimum compensation solution was to place the zeros and poles symmetrically around the crossover frequency. He derived a factor known as K with which the frequencies of the compen- sation zeros and poles may be calculated. K is calculated for the type of compensation selected Figure 17. Type II Compensator G (dB) PHASE –180° –270° fZ fP 0V VRAMP CHF CI RZ RTOP RBOT FROM VOUT VREF EA COMP TO PWM –1 SLO PE –1 SLO PE Figure 17. Type II Compensation To calculate K for Type II compensation use ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ + = 45 2 tan B φ K (32) Values of K between 4 and 15 are practical for implementation, so if the selected type of compensation does not yield a reason- able value of K, try the other type. |
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