SNVAA82 august   2023 LMR38020

 

  1.   1
  2.   Abstract
  3.   Trademarks
  4. 1Introduction
  5. 2Fly-Buck Converter
  6. 3Fly-Buck Basic Operation
    1. 3.1 Basic Intervals of Steady State Operation
    2. 3.2 Impact Of Leakage Inductor On Fly-Buck Operation
  7. 4Design A Fly-Buck Converter with LMR38020
    1. 4.1 IC Select
    2. 4.2 Switching Frequency Set
    3. 4.3 Transformer Design
      1. 4.3.1 Turns Ratio
      2. 4.3.2 Magnetic Inductance
      3. 4.3.3 Check Ipk
    4. 4.4 Output Capacitor Selection
      1. 4.4.1 Primary Output Capacitor
      2. 4.4.2 Secondary Output Capacitor
    5. 4.5 Secondary Output Diode
    6. 4.6 Preload Resistor
  8. 5Bench Test Results
    1. 5.1 Typical Switching Waveforms Under Steady State
    2. 5.2 Start Up
    3. 5.3 Efficiency
    4. 5.4 Load Regulation
    5. 5.5 Short Circuit
    6. 5.6 Thermal Performance
  9. 6Design Considerations
  10. 7Summary
  11. 8References

Impact Of Leakage Inductor On Fly-Buck Operation

In a real circuit, the transformer has leakage inductance and other parasitic inductance or capacitance as shown in Figure 3-2, which can affect the secondary current waveform.

GUID-20230801-SS0I-W5DB-KMZD-F6ZNKRGG4HQH-low.svgFigure 3-2 Fly-Buck Converter Circuit Considering Parasitic

The Figure 3-3 shows the typical current waveform under different levels of leakage inductance(LLK).

When LLK is low, the isec ramps up quickly to charge up COUT2. With larger LLK, isec rises linearly,resulting in larger negative peak current for ipri. If the negative peak current of ipri reaches the negative current limit of the device, the LS will be turned off and the charging to COUT2 will be terminated. Consequently this would result in less energy being transferred to the output and produce lower output voltage.

Therefore, the leakage inductance should be minimized and the maximum duty cycle must be chosen carefully to mitigate these issues. When the secondary output has no load, the turn on of LS can force a small current in the secondary side, and it would gradually charge up COUT2. Since there is no load to discharge COUT2, a net charge will be accumulated on COUT2 and raise the VOUT2 remarkably. In order to prevent this from happening, a preload must be added to the secondary output to help removing the net charge on COUT2 so as to maintain the output voltage at the setting point.

GUID-20230801-SS0I-FBXV-X9QC-0J7MTJQTXKJQ-low.svgFigure 3-3 Current Waveforms Affected by Leakage Inductance