Asynchronous Buck Converter
February 2026 · Source on GitHub
Overview
A 78 × 16 mm two-layer board that takes 12 V in on a barrel jack and puts out 5 V on a USB-A socket at up to 3 A. It works as a bench or car USB supply, and it was my first switching regulator. The goal was to size a converter from the datasheet rather than buy a finished module.
The regulator is an LM2596S-5, a fixed 5 V step-down in TO-263 switching at 150 kHz and rated for 3 A. It is an asynchronous design, meaning a Schottky catch diode carries the freewheel current rather than a second switching FET. That costs efficiency but removes the need for a gate driver and a bootstrap supply.
Why a Switching Regulator
A linear regulator doing 12 V to 5 V at 3 A dissipates (12 - 5) × 3 = 21 W in the package. That is not coolable on a board this size and caps efficiency near 42%. A buck converter stores that energy in an inductor and delivers it to the load instead. Simulation puts this design at 91.3%.
The tradeoff is that a switcher is a layout problem as much as a schematic problem. Every choice below is about either keeping inductor current continuous or keeping the high current loops short.
Component Selection
The target was continuous conduction at the full 3 A load, meaning inductor current never falls to zero during the switching cycle. Discontinuous operation is not dangerous, but it makes output voltage load dependent and worsens ripple.
- L1, 33 µH. Sized from the LM2596 datasheet selection curves for a 12 V input at 3 A. The inductor sets ripple current, which is what determines whether conduction stays continuous.
- C1, 680 µF input. A buck draws input current in pulses rather than smoothly. The input capacitor supplies those pulses locally instead of pulling them down the supply leads, which helps both ripple and EMI.
- C2, 220 µF output. Absorbs inductor ripple current to flatten the 5 V rail, and sets transient response under a load step.
- D1, SS54 Schottky, 40 V and 5 A. The catch diode carries inductor current during the switch off half of the cycle. Schottky for the lower forward drop and fast recovery, with ratings above the 12 V input and 3 A load to cover switching transients.
Layout
Input, switch node, and output traces are widened to 0.8 mm to carry 3 A without meaningful drop or heating. The switch node matters most for noise, since it joins the regulator output pin, the inductor, and the catch diode while swinging the full input voltage at 150 kHz. Kept short it behaves like a trace, and left to sprawl it behaves like an antenna.
The 78 × 16 mm outline is long and narrow so the barrel jack and USB-A socket sit at opposite ends, giving a straight through power path with the switching section in the middle.
Simulation
I modelled the converter in LTspice as an open-loop, fixed-duty stage: an ideal high side switch, the SS54 as the freewheel diode, and the real parasitics that matter, 50 mΩ of inductor series resistance and 50 mΩ of output capacitor ESR. Measurements are averaged over the last millisecond of a 5 ms transient, once the output has settled.
- 91.3% efficiency at the full 3 A load. 16.64 W in, 15.19 W out.
- The catch diode is 62% of the total loss, 0.90 W of 1.45 W. That is the price of an asynchronous design, and it is the first thing a synchronous FET would recover.
- Inductor loss is 0.46 W, another 32%, which leaves only about 6% in the switch and capacitor ESR combined.
- Inductor current never reaches zero. Ripple is 0.63 A peak to peak with a minimum of 2.71 A, so conduction stays continuous at full load, which is what the 33 µH was sized for.
- Output ripple is 31 mV on a 5.03 V rail.
The loss breakdown is the useful part. Knowing the diode dominates tells you where a Rev B would go, and it is a better answer than assuming the regulator itself is the problem.
Status
The schematic and layout are complete in KiCad and the design is simulated. The board has not been fabricated, so the figures above are simulated rather than measured. Once built, the things worth putting on a scope are the switch node waveform, output ripple at full load, and efficiency across the load range against the 91.3% the model predicts.