Porous Absorber Calculator

Model an absorption-coefficient-vs-frequency curve from flow resistivity, thickness, and air gap using the Delany-Bazley-Miki model.

By roomtreatment.diy editorial team ·

Delany-Bazley-Miki porous absorber model — flow resistivity, thickness, and an optional air gap behind the material.

Absorber thickness5cm
Air gap behind absorber0cm
Material · flow resistivity σ
Pa·s/m²
Absorption vs. frequencyNRC ≈ 0.70

NRC ≈ 0.70 for this absorber build.

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How the model works

The Delany-Bazley-Miki model predicts a porous material's characteristic impedance and complex wavenumber from a single measured property: flow resistivity. From those, a transmission-line transform through the layer (optionally over an air gap) to the rigid wall behind it gives the surface impedance, and from that, the absorption coefficient at any frequency.

  • Flow resistivity (σ): higher values mean denser, stiffer material — light fiberglass and rigid mineral wool sit at very different points on the same absorption curve.
  • Thickness: thicker absorbers push the useful absorption band lower in frequency.
  • Air gap: spacing the absorber off the wall extends low-frequency performance without adding material.

Frequently asked questions

What is flow resistivity in acoustic absorbers?
Flow resistivity (σ, in Pa·s/m², also written rayl/m) measures how much a porous material resists airflow through it. It is the single input the Delany-Bazley-Miki model needs to predict a material’s complex characteristic impedance and, from that, its absorption coefficient at any frequency.
Why does an air gap behind a panel improve low-frequency absorption?
An air gap moves the absorber away from the rigid wall, where particle velocity (not pressure) is highest. Because porous absorption works by converting particle velocity into heat via viscous friction, a gap shifts the panel’s peak absorption lower in frequency without adding material thickness.
What is the difference between normal and random incidence absorption?
Normal incidence is the absorption coefficient for sound arriving straight-on (0°). Random (or field/diffuse) incidence averages absorption over every angle a real reverberant room actually presents to a panel, weighted by solid angle (Paris’ formula) — it is usually a better match for published NRC ratings and real-room behavior.