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TPS54010 Datasheet(PDF) 13 Page - Texas Instruments |
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TPS54010 Datasheet(HTML) 13 Page - Texas Instruments |
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13 / 25 page ![]() www.ti.com C8 + 1 2pR1 ƒ LC (20) ƒ ESR0 + 1 2pR ESR C OUT (21) R2 + R1 0.891 V OUT * 0.891 (11) R5 + 1 2pC8 ƒ ESR (22) ƒ Z1 + 1 2pR3C6 (12) ƒ Z2 + 1 2pR1C8 (13) C7 + 1 7pR3 ƒ CO (23) ƒ P1 + 1 2pR5C8 (14) ƒ P2 + 1 2pR3C7 (15) BIAS AND BOOTSTRAP CAPACITORS ƒ INT + 1 2pR1C6 (16) ƒ INT + ƒ CO V IN(MAX) 2 (17) POWER GOOD C6 + 1 2pR1 ƒ INT (18) R3 + 1 p C6 ƒ LC (19) TPS54010 SLVS509A – MAY 2004 – REVISED AUGUST 2004 The closed-loop crossover frequency should be chosen to be greater than fLC and less than one-fifth of the switching frequency. Also, the crossover fre- quency should not exceed 150 kHz, as the error The first pole, fP1 is located to coincide with output amplifier may not provide the desired gain. For this filter ESR zero frequency. This frequency is given by: design, a crossover frequency of 100 kHz was chosen. This value is chosen for comparatively wide loop bandwidth while still allowing for adequate phase boost to insure stability. where RESR is the equivalent series resistance of the output capacitor. Next, calculate the R2 resistor value for the output voltage of 1.5 V using Equation 11: In this case, the ESR zero frequency is 88.4 kHz, and R5 can be calculated from: For any TPS54010 design, start with an R1 value of 10 k Ω. R2 is 14.7 kΩ. The final pole is placed at a frequency above the closed-loop crossover frequency high enough to not Now, the values for the compensation components cause the phase to decrease too much at the that set the poles and zeros of the compensation crossover frequency while still providing enough at- network can be calculated. Assuming that R1 >> than tenuation so that there is little or no gain at the R5 and C6 >> C7, the pole and zero locations are switching frequency. The fP2 pole location for this given by Equation 12 through Equation 18: circuit is set to 3.5 times the closed-loop crossover frequency and the last compensation component value C7 can be derived: Note that capacitors are only available in a limited range of standard values, so the nearest standard value has been chosen for each capacitor. The measured closed-loop response for this design is Additionally, there is a pole at the origin, which has shown in Figure 5. unity gain at a frequency: Every TPS54010 design requires a bootstrap capaci- This pole is used to set the overall gain of the tor, C3, and a bias capacitor, C4. The bootstrap compensated error amplifier and determines the capacitor must be a 0.1 µF. The bootstrap capacitor closed-loop crossover frequency. Because R1 is is located between the PH pins and BOOT. The bias given as 1 k Ω and the crossover frequency is capacitor is connected between the VBIAS pin and selected as 100 kHz, the desired fINT can be calcu- AGND. The value should be 1.0 µF. Both capacitors lated from Equation 17: should be high-quality ceramic types with X7R or X5R grade dielectric for temperature stability. They should be placed as close to the device connection pins as possible. And the value for C6 is given by Equation 18: The TPS54010 is provided with a power-good output pin PWRGD. This output is an open-drain output and is intended to be pulled up to a 3.3-V or 5-V logic The first zero, fZ1 is located at one-half the output supply. A 10-k Ω pullup works well in this application. filter LC corner frequency; so, R3 can be calculated from: The second zero, fZ2 is located at the output filter LC corner frequency; so, C8 can be calculated from: 13 |
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