SLVAFD4 February   2024 TPS54308 , TPS54320 , TPS54350 , TPS54620 , TPS54622 , TPS54821 , TPS54824 , TPS62933F

 

  1.   1
  2.   Abstract
  3.   Trademarks
  4. 1Introduction
  5. 2Components Selection for Secondary Stage Filter
  6. 3Experimental Validation
  7. 4How to Estimate Inductance of Ferrite Bead for Ripple Reduction
  8. 5Summary
  9. 6References
  10. 7Appendix

Components Selection for Secondary Stage Filter

Figure 2-1 shows the scheme of buck converter with second stage filter. A second-order low pass filter is formed by inductor L2 and capacitor C2. A new pair of conjugate poles is introduced with the filter, which can reduce the output voltage ripple and noise at switching frequency through the high frequency gain attenuation. The selection method of inductor L2 and capacitor C2 is analyzed in this section.

GUID-20230616-SS0I-JMGW-P75Z-NCVZ2VDWBG8N-low.svg Figure 2-1 Buck Converter with Second Stage Filter

In several previous studies, the expression of output voltage ripple after the 1st stage LC filter is already derived, as shown in Equation 1. Also see the Output Ripple Voltage for Buck Switching Regulator application note.

Equation 1. V o1-ripple = V o 1- V o V in f sw L r c + 1 8 f sw C o

where, Vo1-ripple is the peak to peak amplitude of output voltage ripple after 1st stage. Vo is output voltage and Vin is input voltage of buck converter. fsw is switching frequency. L and Co are the inductance and capacitance of the 1st stage filter respectively. rc is the ESR of capacitor Co.

The transfer function of second stage filter is shown as Equation 2.

Equation 2. G vv-2nd (s)= R L s 2 R L L 2 C 2 +s L 2 + R L

where RL is output load resistance. Since MLCC is normally used as capacitor C2 to reduce output ripple for second stage, the ESR of C2 is ignored.

A pair of conjugate poles is included in transfer function Equation 2. The poles frequency can be approximately expressed as Equation 3. The loop gain amplitude plot is shown as Figure 2-2.

Equation 3. f 2 1 1 L 2 C 2
GUID-20230616-SS0I-F17X-66DL-GSTLSKS78FPP-low.svg Figure 2-2 Loop Gain Magnitude Plot of Equation (2)

To simplify the relation, the effects of conjugate poles quality factor are ignored and the gain is seen as attenuation with -40dB/dec slope after frequency f2. The relation as Equation 4 can be derived then.

Equation 4. 0dB-20lg A sw lg f 2 -lg f sw =-40dB/dec

where, Asw is the gain amplitude at switching frequency fsw.

The expression of Asw can be derived with Equation 5.

Equation 5. A sw = f 2 2 f sw 2 = 1 4 π 2 f sw 2 L 2 C 2

Applying the attenuation gain Asw on Vo-1ripple, second stage ripple Vo2-ripple is expressed as Equation 6.

Equation 6. V o2-ripple = A sw V o1-ripple = V o 1- V o V in r c + 1 8 f sw C o 4 π 2 f sw 3 L L 2 C 2

To meet the requirement Vo2-ripple≤Vo2-ripple-target, the limitation for the selection of L2 and C2 can be received with Equation 7.

Equation 7. L 2 C 2 V o 1- V o V in r c + 1 8 f sw C o 4 π 2 f sw 3 L V o2-ripple-target

As shown, only the limitation for (L2 x C2) is given in Equation 7, while no limitation is given for L2 and C2 respectively. The inductance and capacitance can be determined with the consideration of BOM cost, DCR loss, and so on.

In Part II of this application note series, the impacts of added passive filter on loop stability can be further analyzed and the components selection range with stability restriction can be further derived then. The completed components selection range and application design method is received by considering both output voltage ripple restriction in this paper and stability restriction in next papers.