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ADP2121 Datasheet(PDF) 17 Page - Analog Devices |
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ADP2121 Datasheet(HTML) 17 Page - Analog Devices |
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17 / 20 page ![]() ADP2121 Rev. B | Page 17 of 20 APPLICATIONS INFORMATION The external component selection for the ADP2121 applica- tions circuit is driven by the load requirement and begins with the selection of the inductor. After the inductor is chosen, CIN and COUT can be selected. Components can be identified using the selection guide and recommended selection tables in this section. INDUCTOR SELECTION The high switching frequency of the ADP2121 allows for minimal output voltage ripple, even with small inductors. Inductor sizing is a trade-off between efficiency and transient response. A small inductor leads to a larger inductor current ripple, which provides better transient response but degrades efficiency. Due to the high switching frequency of the ADP2121, multilayer ceramic inductors can be used for an overall smaller solution size. Shielded ferrite core inductors are recommended for their low core losses and low electromagnetic interference (EMI). As a guideline, the peak-to-peak current ripple of the inductor is typically set to ΔIL = 0.45 × ILOAD (1) where ILOAD is the maximum output current. The largest ripple current, ΔIL, occurs at the maximum input voltage. It is important that the inductor be capable of handling the maximum peak inductor current, IPK, determined by the following equation: IPK = ILOAD(MAX) + ΔIL/2 (2) The dc current rating of the inductor should be greater than the calculated IPK to prevent core saturation. The ADP2121 is designed for applications with a 0.47 µH inductor. Other values are not recommended, and stable operation over all conditions is not guaranteed with their use. Table 6 shows the available 0.47 µH surface-mount inductors that have been tested with the ADP2121. INPUT CAPACITOR SELECTION The input capacitor must be able to support the maximum input operating voltage and the maximum rms input current. Select an input capacitor capable of withstanding the rms input current for the maximum load current in the application using the following equation: IN OUT IN OUT MAX OUT rms V V V V I I ) ( ) ( − × × = (3) The input capacitor reduces the input voltage ripple caused by the switch currents on the VIN pin. Place the input capacitor as close as possible to the VIN pin. In principle, different types of capacitors can be considered, but for battery-powered applications, the best choice is the multilayer ceramic capacitor, due to its small size and low equivalent series resistance (ESR). Table 7 offers suggestions for suitable input capacitors. All capacitors listed in the table are multilayer ceramic capacitors. It is recommended that the VIN pin be bypassed with a 2.2 µF or larger ceramic input capacitor if the supply line has a distri- buted capacitance of at least 10 μF. If not, then at least a 10 μF capacitor is recommended on the input supply pin. The input capacitor can be increased without any limit for better input voltage filtering. X5R or X7R dielectrics with a voltage rating of 6.3 V or 10 V are recommended. Y5U and Z5U dielectrics are not recommended, due to their poor temperature and dc bias characteristics. OUTPUT CAPACITOR SELECTION The output capacitor selection affects both the output voltage ripple and the loop dynamics of the converter. For a given loop crossover frequency (the frequency at which the loop gain drops to 0 dB), the maximum voltage transient excursion (overshoot) is inversely proportional to the value of the output capacitor. The ADP2121 has been designed to operate with small ceramic capacitors in the 4.7 µF to 10 µF range that have low ESR and equivalent series inductance (ESL). These components are able, therefore, to meet stringent output voltage ripple specifications. X5R or X7R dielectrics with a voltage rating of 6.3 V are recommended. Table 8 shows a list of output MLCC capacitors recommended for ADP2121 applications. The minimum effective capacitance required for stable operation is 1.5 µF. When choosing output capacitors, it is also important to account for the loss of capacitance due to output voltage dc bias. This may result in using a capacitor with a higher rated voltage to achieve the desired capacitance value. Additionally, if ceramic output capacitors are used, the capacitor rms ripple current rating should always meet the application requirements. The rms ripple current is calculated as ) ( ) ( ) ( 3 2 1 ) ( MAX IN SW OUT MAX IN OUT rms V f L V V V I COUT × × − × × = (4) At nominal load currents, the converter operates in pulse frequency mode (PFM), and the overall output voltage ripple is the sum of the voltage spike caused by the output capacitor ESR plus the voltage ripple caused by charging and discharging the output capacitor. ΔVOUT = ΔIL × (ESR + 1/(8 × COUT × fSW)) (5) The largest voltage ripple occurs at the highest input voltage. At light load currents, if MODE is set low, then the converter operates in the power-saving mode (PFM), and the output voltage ripple increases. |
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