SNVS624B June 2011 – June 2016 LM3559
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 LM3559 is a synchronous boost flash driver with dual 900-mA high-side current sources. The 2-MHz DC-DC boost regulator allows for the use of small external components. The device operates from a typical input voltage from 2.5 V to 5.5 V and an ambient temperature range of –40°C to +85°C.
COMPONENT | MANUFACTURER | VALUE | PART NUMBER | SIZE | RATING |
---|---|---|---|---|---|
L | Toko | 1 µH | FDSD0312-1R0 | 3 mm × 3 mm × 1.2 mm | 3.3 A |
CIN/COUT | Murata | 10 µF | GRM188R60J106M | 1.6 mm × 0.8 mm × 0.8 mm (0603) | 6.3 V |
LEDs | Lumiled | PWF-4 | VF = 3.6 V at 1 A |
For typical LED flash driver applications, use the parameters listed in Table 19.
DESIGN PARAMETER | EXAMPLE VALUE |
---|---|
Minimum input voltage | 2.5 V |
Minimum output voltage | 1.8 V |
Maximum output voltage | 5 V |
Maximum output current | 1.8 A |
Switching frequency | 2 MHz |
The LM3559 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 converters 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. Therefore, choose the output capacitor 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 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 equivalent series resistance (ESR) of the capacitor (ΔVESR) use Equation 1 and Equation 2:
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 20 lists different manufacturers for various output capacitors and their case sizes suitable for use with the LM3559.
Choosing the correct size and type of input capacitor helps minimize the voltage ripple caused by the switching of the device boost converter, and reduces noise on the input terminal of the boost converter that can feed through and disrupt internal analog signals. In the Figure 43 a 10-µF ceramic input capacitor works well. It is important to place the input capacitor as close as possible to the device input (IN) pin. This reduces the series resistance and inductance that can inject noise into the device due to the input switching currents. Table 20 lists various input capacitors that TI recommends for use with the LM3559.
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 | GRM188R60J06M | 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 LM3559 is designed to use a 1-µH or 2.2-µH inductor. Table 21 lists various inductors and their manufacturers that can work well with the LM3559. When the device is boosting (VOUT > VIN) the inductor typically is 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 must be greater than the maximum operating peak current of the LM3559. This prevents excess efficiency loss that can occur with inductors that operate in saturation and prevents overheating of the inductor and further efficiency loss. For proper inductor operation and circuit performance ensure that the inductor saturation and the peak current limit setting of the LM3559 is greater than IPEAK in Equation 3:
where
MANUFACTURER | L | PART NUMBER | DIMENSIONS (L×W×H) | ISAT | RDC |
---|---|---|---|---|---|
TOKO | 2.2 µH | FDSD0312-H-2R2M | 3 mm × 3.2 mm × 1.2 mm | 2.3 A | 105 mΩ |
TOKO | 1 µH | FDSD0312-H-1R0M | 3 mm × 3.2 mm × 1.2 mm | 3.4 A | 43 mΩ |
TOKO | 1.5 µH | FDSD0312-H-1R5M | 3 mm × 3.2 mm × 1.2 mm | 2.8 A | 71 mΩ |
TOKO | 2.2 µH | FDSD0312-2R2M | 3 mm × 3.2 mm × 1.2 mm | 2.3 A | 145 mΩ |
TOKO | 1 µH | FDSD0312-1R0M | 3 mm × 3.2 mm × 1.2 mm | 3.4 A | 70 mΩ |
TDK | 1 µH | VLS4012ET-1R0N | 4 mm × 4 mm × 1.2 mm | 2.8 A | 50 mΩ |
TDK | 2.2 µH | VLS252012T-2R2M1R3 | 2 mm × 2.5 mm × 1.2 mm | 1.5 A | 130 mΩ |
Flash Brightness Codes 0xBB - 0xFF |
Torch Brightness Codes 0x0F - 0xCF |
Flash Brightness Codes 0x88 - 0xAA |
Torch Brightness Codes 0x00 - 0x04 |
Programming bit [4] of Configuration Register 1 with a 1 selects NTC mode and makes the LEDI/NTC pin a comparator input for flash LED thermal sensing. Figure 48 shows the LM3559 using the NTC thermistor circuit. The thermal sensor resistor divider is composed of R3 and R(T), where R(T) is the Negative Temperature Coefficient Thermistor, VBIAS is the bias voltage for the resistive divider, and R3 is used to linearize the NTC's response around the NTC comparators trip point. CBYP is used to filter noise at the NTC input.
In designing the NTC circuit, we must choose values for VBIAS, R(T) and R3. To begin with, NTC thermistors have a non-linear relationship between temperature and resistance:
where β is given in the thermistor datasheet and R25C is the thermistors value at 25°C. R3 is chosen so that the temperature-to-resistance relationship becomes more linear and can be found by solving for R3 in the R(T) and R3 resistive divider:
where
As an example, with VBIAS = 2.5 V and a thermistor whose nominal value at 25°C is 100 kΩ and a β = 4500 K, the trip point is chosen to be 93°C. The value of R(T) at 93°C is:
Figure 49 shows the linearity of the thermistor resistive divider of the previous example.