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ADP2389ACPZ-R7 数据表(PDF) 14 Page - Analog Devices |
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ADP2389ACPZ-R7 数据表(HTML) 14 Page - Analog Devices |
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14 / 23 page ![]() ADP2389/ADP2390 Data Sheet APPLICATIONS INFORMATION INPUT CAPACITOR SELECTION The input decoupling capacitor attenuates high frequency noise on the input. This capacitor must be a ceramic type in the range of 10 µF to 47 µF. Place the capacitor close to the PVIN pin. Keep the loop composed by this input capacitor, high-side MOSFET and low-side MOSFET as small as possible. The voltage rating of the input capacitor must be greater than the maximum input voltage. The rms current rating of the input capacitor must be larger than the value calculated from the following equation: ( ) D D I I OUT RMS CIN – 1 _ × × = where: IOUT is the output current. D is the duty cycle. OUTPUT VOLTAGE SETTING An external resistor divider sets the output voltages of the ADP2389/ADP2390. Calculate the resistor values using the following equation: + × = BOT TOP OUT R R V 1 6 . 0 where : RTOP is the top feedback resistor. RBOT is the bottom feedback resistor. To limit output voltage accuracy degradation due to FB bias current (0.1 µA maximum) to less than 0.5% (maximum), ensure that RBOT is less than 30 kΩ. Table 5 gives the recommended resistor divider for various output voltages. Table 5. Resistor Divider for Difference Output Voltage VOUT (V) RTOP, ±1% (kΩ) RBOT, ±1% (kΩ) 1.0 10 15 1.2 10 10 1.5 15 10 1.8 20 10 2.5 47.5 15 3.3 10 2.21 5.0 22 3 INDUCTOR SELECTION The inductor value is determined by the operating frequency, the input voltage, output voltage, and inductor ripple current. Using a small inductor leads to a faster transient response; however, it degrades efficiency due to its larger inductor ripple current. Using a large inductor value leads to smaller ripple current and better efficiency but results in a slower transient response. As a guideline, the inductor ripple current, ΔIL, is typically set to one third of the maximum load current. Calculate the inductor value using the following equation: SW L OUT IN f I D V V L × ∆ × = ) – ( where: VIN is the input voltage. VOUT is the output voltage. D is the duty cycle. ΔIL is the inductor ripple current. fSW is the switching frequency. IN OUT V V D = The peak inductor current (IPEAK) is calculated using 2 L OUT PEAK I I I ∆ + = The saturation current of the inductor must be greater than the peak inductor current. For the ferrite core inductors with a quick saturation characteristic, the saturation current rating (ISAT) of the inductor must be greater than the current-limit threshold of the switch to prevent the inductor from being saturated. Calculate the rms current of the inductor (IRMS) from 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 6 lists recommended inductors. Table 6. Recommended Inductors Vendor Device No. Value (µH) ISAT (A) IRMS (A) DCR (mΩ) CoilCraft XAL7030-102ME 1 21.8 16.1 4.55 XAL7030-152ME 1.5 11.9 23.5 7.6 XAL7030-222ME 2.2 10 18 13.7 Toko FDUE1040D-H-R22M 0.22 32 32 0.64 FDUE1040D-H-R45M 0.45 27 24 1.02 FDU1040D-H-R68M 0.68 21 20 1.7 FDUE1040D-H-1R0M 1.0 18 16 2.35 FDA1254-H-1R2M 1.2 20.2 18.4 2.6 Würth Elektronik 744 333 0022 0.22 60 21.5 0.6 744 333 0047 0.47 47 20 0.8 744 333 0068 0.68 38 20 1.35 744 333 0082 0.82 36 20 1.35 744 332 0100 1.0 27.5 20 1.35 744 325 120 1.2 25 20 1.8 744 333 0150 1.5 27 18 2.5 744 333 0220 2.2 22 16 3.7 Rev. 0 | Page 14 of 23 |
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