
D = VOUT + VSW_BOT + IOUT x RDC
VIN + VSW_BOT - VSW_TOP
Iirrms = I(I2d)I(Id1)I(I 21
2
av2
2
av1 -++-+- 3d)I 2
av
21
LM26420-Q1
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SNVSB35B –MAY 2018–REVISED JUNE 2020
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When selecting an inductor, make sure that it is capable of supporting the peak output current without saturating.
Inductor saturation results in a sudden reduction in inductance and prevents the regulator from operating
correctly. The peak current of the inductor is used to specify the maximum output current of the inductor and
saturation is not a concern due to the exceptionally small delay of the internal current limit signal. Ferrite based
inductors are preferred to minimize core losses when operating with the frequencies used by the LM26420-Q1.
This presents little restriction because the variety of ferrite-based inductors is huge. Lastly, inductors with lower
series resistance (RDCR) provides better operating efficiency. For recommended inductors, see Table 2.
8.2.1.2.3 Input Capacitor Selection
The input capacitors provide the AC current needed by the nearby power switch so that current provided by the
upstream power supply does not carry a lot of AC content, generating less EMI. To the buck regulator in
question, the input capacitor also prevents the drain voltage of the FET switch from dipping when the FET is
turned on, therefore, providing a healthy line rail for the LM26420-Q1 to work with. Because typically most of the
AC current is provided by the local input capacitors, the power loss in those capacitors can be a concern. In the
case of the LM26420-Q1 regulator, because the two channels operate 180° out of phase, the AC stress in the
input capacitors is less than if they operated in phase. The measure for the AC stress is called input ripple RMS
current. It is strongly recommended that at least one 10-µF ceramic capacitor be placed next to each of the VIND
pins. Bulk capacitors such as electrolytic capacitors or OSCON capacitors can be added to help stabilize the
local line voltage, especially during large load transient events. As for the ceramic capacitors, use X7R or X5R
types. They maintain most of their capacitance over a wide temperature range. Try to avoid sizes smaller than
0805. Otherwise significant drop in capacitance can be caused by the DC bias voltage. See the Output Capacitor
section for more information. The DC voltage rating of the ceramic capacitor must be higher than the highest
input voltage.
Capacitor temperature is a major concern in board designs. While using a 10-µF or higher MLCC as the input
capacitor is a good starting point, it is a good idea to check the temperature in the real thermal environment to
make sure the capacitors are not overheated. Capacitor vendors can provide curves of ripple RMS current
versus temperature rise based on a designated thermal impedance. In reality, the thermal impedance can be
very different, so it is always a good idea to check the capacitor temperature on the board.
Because the duty cycles of the two channels can overlap, calculation of the input ripple RMS current is a little
tedious — use Equation 14:
where
• I1is the maximum output current of Channel 1
• I2is the maximum output current of Channel 2
• d1 is the non-overlapping portion of the duty cycle, D1, of Channel 1
• d2 is the non-overlapping portion of the duty cycle, D2, of Channel 2
• d3 is the overlapping portion of the two duty cycles
• Iav is the average input current (14)
Iav = I1× D1+ I2× D2. To quickly determine the values of d1, d2, and d3, refer to the decision tree in Figure 36.
To determine the duty cycle of each channel, use D = VOUT / VIN for a quick result or use Equation 15 for a more
accurate result.
where
• RDC is the winding resistance of the inductor (15)
Example:
• VIN =5V
• VOUT1 = 3.3 V
• IOUT1 =2A
• VOUT2 = 1.2 V
• IOUT2 = 1.5 A
• RDS = 170 mΩ