SLVSB38C March 2011 – August 2016 TPS62242-Q1
PRODUCTION DATA.
NOTE
Information in the following applications sections is not part of the TI component specification, and TI does not warrant its accuracy or completeness. TI’s customers are responsible for determining suitability of components for their purposes. Customers should validate and test their design implementation to confirm system functionality.
The TPS62242-Q1 device is a high-efficiency synchronous step-down DC-DC converter featuring power save mode.
The device operates over an input voltage range from 2 V to 6 V.
Table 2 shows the list of components for the Application Curves. Users must verify and validate these components for suitability with their application before using the components.
VALUE | COMPONENT REFERENCE | PART NUMBER | MANUFACTURER |
---|---|---|---|
4.7 μF, 6.3 V. X5R Ceramic | CIN | GRM188R60J475K | Murata |
10 μF, 6.3 V. X5R Ceramic | COUT | GRM188R60J106M | Murata |
22 pF, COG Ceramic | C1 | Murata | |
2.2 μH, 110 mΩ | L1 | LPS3015 | Coilcraft |
The TPS62242-Q1 device is designed to operate with inductors in the range of 1.5 μH to 4.7 μH and with output capacitors in the range of 4.7 μF to 22 μF. The device is optimized for operation with a 2.2-μH inductor and 10‑μF output capacitor.
Larger or smaller inductor values can be used to optimize the performance of the device for specific operation conditions. For stable operation, the L and C values of the output filter may not fall below 1-μH effective Inductance and 3.5-μF effective capacitance. Selecting larger capacitors is less critical, because the corner frequency of the L-C filter moves to lower frequencies with fewer stability problems.
The inductor value has a direct effect on the ripple current. The selected inductor must be rated for its DC resistance and saturation current (Table 3). The inductor ripple current (ΔIL) decreases with higher inductance and increases with higher VI or VO.
The inductor selection also has an impact on the output voltage ripple in the PFM mode. Higher inductor values lead to lower-output voltage ripple and higher PFM frequency, and lower inductor values lead to a higher-output voltage ripple with lower PFM frequency.
Equation 2 calculates the maximum inductor current in PWM mode under static load conditions. The saturation current of the inductor should be rated higher than the maximum inductor current as calculated with Equation 3. This is the recommendation because during heavy-load transients the inductor current rises above the calculated value.
where
A more conservative approach is to select the inductor current rating just for the maximum switch current limit ILIMF of the converter.
Accepting larger values of ripple current allows the use of low inductance values, but results in higher output voltage ripple, greater core losses, and lower output current capability.
The total losses of the coil strongly impact the efficiency of the DC-DC conversion and consist of both the losses in the DC resistance (R(DC)) and the following frequency-dependent components:
INDUCTANCE (μH) | DIMENSIONS (mm) | PART NUMBER | MANUFACTURER |
---|---|---|---|
2 | 2.5 × 2 × 1 | MIPS2520D2R2 | FDK |
2 | 2.5 × 2 × 1.2 | MIPSA2520D2R2 | FDK |
2.2 | 2.5 × 2 × 1 | KSLI-252010AG2R2 | Hitachi Metals |
2.2 | 2.5 × 2 × 1.2 | LQM2HPN2R2MJ0L | Murata |
2.2 | 3 × 3 × 1.4 | LPS3015 | Coilcraft |
The advanced fast-response voltage-mode control scheme of the TPS62242-Q1 device allows the use of tiny ceramic capacitors. Ceramic capacitors with low-ESR values have the lowest-output voltage ripple and are recommended. The output capacitor requires either an X7R or X5R dielectric. Y5V and Z5U dielectric capacitors, aside from their wide variation in capacitance over temperature, become resistive at high frequencies.
At nominal load current, the device operates in PWM mode and the RMS ripple current is calculated as in Equation 4:
At nominal load current, the device operates in PWM mode 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 as in Equation 5:
At light load currents, the converter operates in power save mode and the output voltage ripple depends on the output capacitor and inductor value. Larger output capacitor and inductor values minimize the voltage ripple in PFM mode and tighten DC output accuracy in PFM mode.
The buck converter has a natural pulsating input current; therefore, a low-ESR input capacitor is required for best input voltage filtering and minimizing the interference with other circuits caused by high-input voltage spikes. For most applications, a 4.7-μF to 10-μF ceramic capacitor is recommended (Table 4). Because ceramic capacitors lose up to 80% of their initial capacitance at 5 V, TI recommends using a 10-μF input capacitor for input voltages greater than 4.5 V. The input capacitor can be increased without any limit for better input voltage filtering.
Take care when using only small ceramic input capacitors. When a ceramic capacitor is used at the input, and the power is being supplied through long wires, such as from a wall adapter, a load step at the output, or VIN step on the input, can induce ringing at the VIN pin. The ringing can couple to the output and be mistaken as loop instability, or could even damage the part by exceeding the maximum ratings.
CAPACITANCE (µF) | DIMENSIONS (mm) | PART NUMBER | MANUFACTURER |
---|---|---|---|
4.7 | 0603: 1.6 × 0.8 × 0.8 | GRM188R60J475K | Murata |
10 | 0603: 1.6 × 0.8 × 0.8 | GRM188R60J106M69D | Murata |