How it works
The holes' open area, the panel thickness, and the cavity depth set the resonance; a porous fill damps and widens it. Fresnelcut picks the geometry for your target band and reports the peak absorption estimate plus the backing materials to buy. It is the drilled-hole sibling of the slat absorber.
Worked example: 5 mm holes on a 20 mm grid
Take a 6 mm panel drilled with 5 mm holes on a 20 mm square pitch, over a 50 mm cavity. The open-area ratio is p = π·5² / (4·20²) ≈ 0.0491 — about 5% open. The effective hole length adds roughly 0.8 × the hole diameter to the panel thickness for the end correction:
t_eff ≈ t + 0.8d = 6 + 4 = 10 mmWith t_eff = 10 mm and D = 50 mm, f_res = (343.2/2π)·√(0.0491/(0.010·0.050)) ≈ 541 Hz. Open this build in the designer to retarget it to your own frequency — Fresnelcut solves the hole size, pitch, and cavity depth together rather than making you iterate by hand.
What you'll need to build it
A laser or CNC router makes short work of a repeating hole grid — this is usually the faster of the two absorber types to cut. As with the slat absorber, the holes alone give a narrow resonance; a porous fill or resistive facing in the cavity behind the panel is what turns that into a usefully broad absorption band, and Fresnelcut's bill of materials specifies it alongside the panel geometry.
Perforated vs. slat
Same resonant-absorber physics, different opening shape. A round-hole grid is typically the quicker cut and reads as a cleaner, more uniform surface; the slat absorber's parallel slots are the more traditional wood-slat look and are easy to cut without a laser or CNC at all.
Getting the target frequency right
As with the slat absorber, the three levers here — hole open-area ratio, effective hole length, and cavity depth — interact, so hole diameter and pitch are usually fixed to whatever's practical to drill or laser-cut, and the cavity depth is solved to hit the target frequency. Smaller, more closely-spaced holes push the open-area ratio and the end correction in opposite directions, which is why hand-picking a hole pattern for a specific frequency is fiddly compared to letting the geometry solve for it.
Finishing and mounting
The drilled face is the visible surface, so sand and finish it before assembly — paint or veneer over the holes afterward risks partially closing them and shifting the open-area ratio away from what was designed. Mount the finished panel with a standoff equal to the cavity depth solved above; mounting it flush to the wall removes the cavity entirely and the resonance won't land where the calculator said it would.
f_res = (c / 2π) · √( p / (t_eff · D) )p = hole open-area ratio, t_eff = effective hole length (with end correction), D = cavity depth.
Best for
- Low-mid resonance and boxiness
- A clean, uniform look that's simple to fabricate
Not the tool for
- High-frequency echo (use a diffuser)
- Deep bass without a large cavity