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Source: https://jmrplens.github.io/phonometry/materials/diffusers/

# Diffusers and surfaces

Where the [Absorbers](https://jmrplens.github.io/phonometry/absorbers/) subsection asks
how much energy a material removes from the field, this one asks what a
*surface* does with the sound it returns: how much it throws off the specular
direction and how evenly it spreads it. Two guides walk that ground, and a
third family of surface measurements — pavements characterised where they lie —
has its own subsection nested inside this group.

[Diffusers and Their Coefficients](https://jmrplens.github.io/phonometry/materials/diffusers/) is the
measurement and design core: the random-incidence **scattering coefficient**
$s$ of ISO 17497-1, measured on a reverberation-room turntable, the
**diffusion coefficient** $d$ of ISO 17497-2, measured on a free-field
goniometer, the Schroeder quadratic-residue design rules with the Fraunhofer
far-field prediction that grades a well-depth sequence before it is built,
and the closing argument for why the two coefficients must never be swapped.

[Metadiffusers](https://jmrplens.github.io/phonometry/materials/metadiffusers/) shrinks the Schroeder
diffuser by an order of magnitude: slits loaded by Helmholtz resonators slow
the sound until a 2 cm panel reproduces the reflection phases of wells 27 cm
deep, with critical coupling supplying the perfectly absorbing `0` state that
ternary sequences need. The published quadratic-residue design is evaluated
end to end, transfer-matrix chain to FDTD cross-check.

[Surfaces measured in place](https://jmrplens.github.io/phonometry/surfaces/) takes the
absorption question outdoors, to the surfaces that have no sample: it covers
the ISO 13472-1 subtraction technique and the ISO 13472-2 spot tube, and the
decision between them.

The neighbours are close: the diffuser panels are surface relatives of the
[metamaterial absorbers](https://jmrplens.github.io/phonometry/absorbers/metamaterial-absorbers/) built
from the same slit and resonator cell, the scattering coefficient feeds the
room predictions of
[Room acoustics](https://jmrplens.github.io/phonometry/buildings/rooms/), and the road
methods serve the outdoor-noise interest of
[Environment and transport](https://jmrplens.github.io/phonometry/environment/).

## Pages in this section

- [Diffusers and Their Coefficients](https://jmrplens.github.io/phonometry/materials/diffusers/): the
  ISO 17497-1 scattering and ISO 17497-2 diffusion coefficients, Schroeder
  design and the far-field prediction model.
- [Metadiffusers](https://jmrplens.github.io/phonometry/materials/metadiffusers/): deep-subwavelength
  Schroeder diffusers from resonator-loaded slits, with slow sound and
  ternary sequences.

## See also

Pages elsewhere on the site that this section leans on:

- [Surfaces measured in place](https://jmrplens.github.io/phonometry/surfaces/) and its guide
  [In-situ Road-Surface Absorption](https://jmrplens.github.io/phonometry/surfaces/road-absorption/):
  the ISO 13472-1 subtraction technique and the ISO 13472-2 spot method.

## What this section does not cover

Both prediction models here are **design estimates, not measurements**. The
Fraunhofer far field the diffuser and metadiffuser pages share loses accuracy
at low frequency, at grazing angles and over strongly absorbing surfaces, and
it ignores edge diffraction, so it grades a well-depth sequence before it is
built and does not replace an ISO 17497-2 measurement; the metadiffuser model
is locally reacting on top of that, with no coupling between wells. Only the
quadratic-residue depth sequence has a dedicated helper — primitive-root and
modulated arrangements are discussed as design guidance and enter through the
explicit depth or reflection arguments. The inverse problem, solving resonator
geometries for a target phase profile, is not automated: the workflow matches
phases by evaluation. On the measurement side the library reduces the data but
does not run the rig: the ISO 17497-1 turntable and the ISO 17497-2 goniometer
supply the reverberation times and the polar response, and what is implemented
is the arithmetic that turns them into a coefficient.
