SLUAAG5 March   2022 TPS62933

 

  1.   Trademarks
  2. 1Introduction
  3. 2Cff in High-Output Voltage Internally Compensated PCM Buck Converter
  4. 3Effects of Cff on the Loop
  5. 4Method for Selecting Cff
  6. 5Experimental Verification for TPS62933
  7. 6Summary
  8. 7References
  9.   A Validation Results for the Proposed Method

Method for Selecting Cff

This method is implemented by letting the loop gain cross 0 dB with –20 dB/dec slope. To be noted, –20 dB/dec gain at 0 dB is not a necessary condition for stability. So this method just provides an allowable range for Cff and it does not mean the converter will be unstable if Cff exceeds this range.

For the case as Figure 4-1(a) shows, when the EA zero frequency fZ_EA is larger than bandwidth, the Cff zero fz can be added inside bandwidth, then the loop gain can cross 0 dB with –20 dB/dec, as Figure 4-1(b) shows.

Figure 4-1 Correct Method to use Cff by Only Adding Cff Zero Inside Bandwidth

As the case in Figure 4-2 shows, the zero and pole introduced by Cff are both added inside bandwidth and the system stability can still be ensured. Although the slope of loop gain becomes –40 dB/dec again after the pole fp, the increase in loop gain with Cff makes the bandwidth increase and the fZ_EA becomes smaller than the bandwidth. A –20-dB/dec crossing is achieved and the system has enough phase margin.

Figure 4-2 Correct Method to use Cff by Adding Both the Cff Zero and Pole Inside Bandwidth

As the case in Figure 4-3 shows, both the zero and pole introduced by Cff are inside bandwidth, but the EA zero frequency fZ_EA is still larger than the bandwidth. At this condition, the loop gain will still cross 0 dB with –40 dB/dec, which cannot ensure the system phase margin.

Figure 4-3 Incorrect Method to use Cff by Adding Both the Cff Zero and Pole Inside Bandwidth

Therefore, the two restrictions deduced to achieve a stable state with –20 dB/dec crossing after adding feedforward capacitor are (1) fz < fc, and (2) avoiding the condition as exhibited in Figure 4-3. fc is the gain crossover frequency when not adding Cff.

The expression of fc has already been derived in Part I, as shown in Equation 7.

Equation 7.

With the restriction fz < fc, the low limit of Cff is obtained based on Equation 5 and Equation 7:

Equation 8.

This equation corresponds to the limit for restriction 1. Since Equation 9 corresponds to the condition as Figure 4-3(b), restriction 2 to avoid that condition corresponds to Equation 10.

Equation 9.
Equation 10.

where Ap is the amplitude of gain at fp.

To get the expressions of Ap and fcross, first determine the relation between gain and frequency as Equation 11, Equation 12, and Equation 13.

Equation 11.
Equation 12.
Equation 13.

Next, the expressions of Ap and fcross as Equation 14 and Equation 15 are determined.

Equation 14.
Equation 15.

Substituting expressions for AP_OUT, fP_OUT, fz, and fp into Equation 14 and Equation 15, then Equation 16 is calculated as the equation for restriction 2 based on Equation 10, Equation 14, and Equation 15.

Equation 16.

Combining Equation 8 for restriction 1 and Equation 16 for restriction 2, Equation 17 and Equation 18 are the limits for Cff.

Equation 17.
Equation 18.