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ADP5014ACPZ-R7 数据表(PDF) 23 Page - Analog Devices |
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ADP5014ACPZ-R7 数据表(HTML) 23 Page - Analog Devices |
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23 / 34 page ![]() Data Sheet ADP5014 Rev. A | Page 23 of 34 The maximum output voltage for a given input voltage and switching frequency is limited by the minimum off time or the maximum duty cycle. The minimum off time for each channel is 50 ns (typical). The maximum output voltage for a given input voltage and switching frequency is calculated using the following equation: VOUT_MAX = VIN × (1 − tMIN_OFF × fSW) − (RDSON1 − RDSON2) × IOUT_MAX × (1 − tMIN_OFF × fSW) − (RDSON2 + RL) × IOUT_MAX (2) where: VOUT_MAX is the maximum output voltage. tMIN_OFF is the minimum off time. fSW is the switching frequency. RDSON1 is the high-side MOSFET on resistance. RDSON2 is the low-side MOSFET on resistance. IOUT_MAX is the maximum output current. RL is the resistance of the output inductor. As shown in Equation 1 and Equation 2, reducing the switching frequency eases the minimum on time and off time limitations. CURRENT-LIMIT SETTING The ADP5014 has two selectable current-limit thresholds for each channel. Ensure that the selected current-limit value is larger than the peak current of the inductor, IPEAK. See Table 6 for the current-limit configuration for each channel. SOFT START SETTING The buck regulators in the ADP5014 include soft start circuitry that ramps the output voltage in a controlled manner during startup, thereby limiting the inrush current. To set the soft start time to a value of 2 ms or 16 ms, connect a resistor from the CFG2 pin to the ground (see the Soft Start section). INDUCTOR SELECTION The inductor value is determined by the operating frequency, input voltage, output voltage, and inductor ripple current. Using a small inductor yields faster transient response but degrades efficiency due to the larger inductor ripple current. Using a large inductor value yields a smaller ripple current and better efficiency, but results in slower transient response. Therefore, a trade-off must be made between the transient response and efficiency. As a guideline, the inductor ripple current, ΔIL, is typically set to a value from 30% to 40% of the maximum load current. The inductor value is calculated using the following equation: L = [(VIN − VOUT) × D]/(ΔIL × fSW) where: VIN is the input voltage. VOUT is the output voltage. D is the duty cycle (D = VOUT/VIN). ΔIL is the inductor ripple current. fSW is the switching frequency. The ADP5014 has internal slope compensation in the current loop to prevent subharmonic oscillations when the duty cycle is greater than 50%.The inductor peak current is calculated using the following equation: IPEAK = IOUT + (ΔIL/2) The saturation current of the inductor must be larger than the peak inductor current. For ferrite core inductors with a fast saturation characteristic, the saturation current rating of the inductor are higher than the current-limit threshold of the buck regulator to prevent the inductor from becoming saturated. The rms current of the inductor is calculated using the following equation: 12 2 2 L OUT RMS I I I ∆ + = Shielded ferrite core materials are recommended for low core loss and low electromagnetic interference (EMI). Table 11 lists the recommended inductors. Table 11. Recommended Inductors Vendor Part No. Value (µH) ISAT (A) IRMS (A) DCR (mΩ) Size (mm) Coilcraft XAL4020-601 0.6 10.4 11.7 9.5 4 × 4 XAL4020-102 1.0 8.7 9.6 13.3 4 × 4 XAL4020-152 1.5 7.1 7.5 21.5 4 × 4 XAL4020-222 2.2 5.6 5.5 35.2 4 × 4 TOKO DFE252012P-R68M 0.68 5.3 4.1 30 2.5 × 2.0 DFE252012P-1R0P 1.0 4.8 3.8 35 2.5 × 2.0 DFE252012P-1R5P 1.5 3.9 3.0 50 2.5 × 2.0 DFE252012P-2R2P 2.2 3.4 2.6 70 2.5 × 2.0 Wurth 744383560068 0.68 9.4 8.2 7.5 4.1 × 4.1 74438356010 1 9.0 7.2 12 4.1 × 4.1 74438356015 1.5 7.8 5.8 15 4.1 × 4.1 74438356022 2.2 6.2 4.7 29 4.1 × 4.1 |
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