JAJSLH2 March 2021 TPS62810M , TPS62811M , TPS62812M , TPS62813M
PRODUCTION DATA
The TPS6281xM device is designed for a nominal 0.47-µH inductor with a typical switching frequency of 2.25 MHz. Larger values can be used to achieve a lower inductor current ripple, but they can have a negative impact on efficiency and transient response. Smaller values than 0.47 µH cause a larger inductor current ripple, which causes larger negative inductor current in forced PWM mode at low or no output current. For a higher or lower nominal switching frequency, the inductance must be changed accordingly.
The inductor selection is affected by several effects like the following:
where
TYPE | INDUCTANCE [µH] | CURRENT [A] (1) | FOR DEVICE | NOMINAL SWITCHING FREQUENCY | DIMENSIONS [LxBxH] mm | MANUFACTURER(2) |
OPERATION AT –55°C |
---|---|---|---|---|---|---|---|
ML433PYA601MLZ | 0.6 µH, ±20% | 10.4 | TPS62810M, TPS62813M, TPS62812M | 2.25 MHz | 4 × 4 × 2.1 | Coilcraft |
yes |
ML433PYA401MLZ | 0.4 µH, ±20% | 12.5 | TPS62810M, TPS62813M, TPS62812M | 2.25 MHz | 4 × 4 × 2.1 | Coilcraft |
yes |
XFL4015-471ME | 0.47 µH, ±20% | 3.5 | TPS62813M, TPS62812M | 2.25 MHz | 4 × 4 × 1.6 | Coilcraft |
no |
XEL4020-561ME | 0.56 µH, ±20% | 9.9 | TPS62810M, TPS62813M, TPS62812M | 2.25 MHz | 4 × 4 × 2.1 | Coilcraft |
no |
XEL4030-471ME | 0.47 µH, ±20% | 12.3 | TPS62810M, TPS62813M, TPS62812M | 2.25 MHz | 4 × 4 × 3.1 | Coilcraft |
no |
XEL3515-561ME | 0.56 µH, ±20% | 4.5 | TPS62813M, TPS62812M | 2.25 MHz | 3.5 × 3.2 × 1.5 | Coilcraft |
no |
XFL3012-331MEB | 0.33 µH, ±20% | 2.6 | TPS62811M, TPS62812M | ≥ 3.5 MHz | 3 × 3 × 1.3 | Coilcraft |
no |
XPL2010-681ML | 0.68 µH, ±20% | 1.5 | TPS62811M | 2.25 MHz | 2 × 1.9 × 1 | Coilcraft |
no |
DFE252012PD-R47M | 0.47 µH, ±20% | see data sheet | TPS62811M, TPS62813M, TPS62812M | 2.25 MHz | 2.5 × 2 × 1.2 | Murata |
no |
Calculating the maximum inductor current using the actual operating conditions gives the minimum saturation current of the inductor needed. A margin of about 20% is recommended to add. A larger inductor value is also useful to get lower ripple current, but increases the transient response time and size as well.