SNVS891H September 2012 – September 2015 LM3642
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 LM3642 can drive one flash LED at currents up to 1.5 A. The 4-MHz DC-DC boost regulator allows for the use of small value discrete external components.
Example requirements based on default register values:
DESIGN PARAMETER | EXAMPLE VALUE |
---|---|
Input voltage range | 2.5 V to 5.5 V |
Brightness control | I2C Register |
LED configuration | 1 Flash LED |
Boost switching frequency | 4 MHz |
Flash brightness | 1.5 A maximum |
COMPONENT | MANUFACTURER | VALUE | PART NUMBER | SIZE | CURRENT/VOLTAGE RATING (RESISTANCE) |
---|---|---|---|---|---|
L | TOKO | 1 µH | DFE201610C | 2 mm × 1.6 mm × 1 mm | 2.5 A |
COUT | Murata | 10 µF | GRM188R60J106M | 1.6 mm × 0.8 mm × 0.8 mm (0603) | 6.3 V |
CIN | |||||
LED | Lumiled | PWF-4 | VF = 3.6 V, @1.5 A |
The LM3642 is designed to operate with at least a 10-µF ceramic output capacitor. When the boost converter is running the output capacitor supplies the load current during the boost converter's on-time. When the NMOS switch turns off the inductor energy is discharged through the internal PMOS switch, supplying power to the load and restoring charge to the output capacitor. This causes a sag in the output voltage during the on-time and a rise in the output voltage during the off-time. The output capacitor is therefore chosen to limit the output ripple to an acceptable level depending on load current and input/output voltage differentials and also to ensure the converter remains stable.
For proper operation the output capacitor must be at least a 10-µF ceramic. Larger capacitors such as a 22-µF capacitor or capacitors in parallel can be used if lower output voltage ripple is desired. To estimate the output voltage ripple considering the ripple due to capacitor discharge (ΔVQ) and the ripple due to the capacitors ESR (ΔVESR) use the following equations:
For continuous conduction mode, the output voltage ripple due to the capacitor discharge is:
The output voltage ripple due to the output capacitors ESR is found by:
In ceramic capacitors the ESR is very low so a close approximation is to assume that 80% of the output voltage ripple is due to capacitor discharge and 20% from ESR. Table 4 lists different manufacturers for various output capacitors and their case sizes suitable for use with the LM3642.
Choosing the correct size and type of input capacitor helps minimize the voltage ripple caused by the switching of the LM3642 device’s boost converter, and reduces noise on the boost converter's input terminal that can feed through and disrupt internal analog signals. In the typical application circuit a 10-µF ceramic input capacitor works well. It is important to place the input capacitor as close as possible to the LM3642 device’s input (IN) pin. This reduces the series resistance and inductance that can inject noise into the device due to the input switching currents. Table 4 lists various input capacitors that are recommended for use with the LM3642.
MANUFACTURER | PART NUMBER | VALUE | CASE SIZE | VOLTAGE RATING |
---|---|---|---|---|
TDK Corporation | C1608JB0J106M | 10 µF | 0603 (1.6 mm × 0.8 mm × 0.8 mm) | 6.3 V |
TDK Corporation | C2012JB1A106M | 10 µF | 0805 (2 mm × 1.25 mm × 1.25 mm) | 10 V |
TDK Corporation | C2012JB0J226M | 22 µF | 0805 (2 mm × 1.25 mm × 1.25 mm) | 6.3 V |
Murata | GRM188R60J106M | 10 µF | 0603 (1.6 mm × 0.8 mm × 0.8 mm) | 6.3 V |
Murata | GRM21BR61A106KE19 | 10 µF | 0805 (2 mm × 1.25 mm × 1.25 mm) | 10 V |
Murata | GRM21BR60J226ME39L | 22 µF | 0805 (2 mm × 1.25 mm × 1.25 mm) | 6.3 V |
The LM3642 is designed to use a 1-µH or 0.47-µH inductor. Table 5 lists various inductors and their manufacturers that can work well with the LM3642. When the device is boosting (VOUT > VIN) the inductor will typically be the largest area of efficiency loss in the circuit. Therefore, choosing an inductor with the lowest possible series resistance is important. Additionally, the saturation rating of the inductor should be greater than the maximum operating peak current of the LM3642. This prevents excess efficiency loss that can occur with inductors that operate in saturation. For proper inductor operation and circuit performance, ensure that the inductor saturation and the peak current limit setting of the LM3642 are greater than IPEAK in the following calculation:
where ƒSW = 4 MHz, and efficiency can be found in the Typical Characteristics plots.
MANUFACTURER | L | PART NUMBER | DIMENSIONS (L×W×H) | ISAT | RDC |
---|---|---|---|---|---|
TOKO | 1 µH | DFE252010C | 2.5 mm × 2 mm × 1 mm | 2.7 A | 78 mΩ |
TOKO | 1 µH | DFE252012C | 2.5 mm × 2 mm × 1.2 mm | 3 A | 59 mΩ |
TOKO | 0.47 µH | DFE201612C | 2 mm × 1.6 mm × 1.2 mm | 3.4 A | 82 mΩ |
TOKO | 1 µH | DFE201610C | 2 mm × 1.6 mm × 1 mm | 2.5 A | 79 mΩ |