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Revision as of 17:17, 27 June 2023 by Aumann (talk | contribs)

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Figure 1: Sketch of the geometry. The porous material is marked in blue, the acoustic source by q.
Figure 2: Frequency response function.

Description

The Porous absorber benchmark models the sound pressure in a cavity excited by a single harmonic load. One side of the cavity is covered by a layer of poroelastic material, which adds dissipation to the system. The geometry of this model follows [1]. Various projection-based model order reduction methods have been applied and compared using this example as a benchmark in [2].

The cavity has the dimensions 0.75 \times 0.6 \times 0.4\,\mathrm{m} and one wall is covered by a 0.05\,\mathrm{m} thick poroelastic layer acting as a sound absorber. The poroelastic material is described by the Biot theory[3] and the system is excited by a point source located in a corner opposite of the porous layer. The material parameters for the acoustic fluid and the poroelastic material have been chosen according to[1].

Dimensions

System structure:


\begin{align}
\left( A_1 + \tilde{\gamma}(s) A_2 + \tilde{\rho}_f(s) A_3 + s^2 A_4 + s^2 \tilde{\gamma}(s) A_5 + s^2 \tilde{\rho}(s) A_6 + \frac{s^2 \phi^2}{\tilde{R}(s)} A_7 \right) x(s) &= B, \\
y(s) &= C x(s),
\end{align}

with the frequency dependent functions for the effective densities \tilde{\rho}(s), \tilde{\rho}_f(s), the parameter \tilde{\gamma}(s) relating the effective densities and the frequency dependent elasticity coefficients to the porosity, and the scaled effective bulk modulus \tilde{R}(s). For more details on the functions, see [1].


System dimensions:

A_i, \in \mathbb{R}^{n \times n}, with i=1, \ldots, 7 , B \in \mathbb{R}^{n \times 1}, C \in \mathbb{R}^{1 \times n}, with n=386\,076.


Data

The data is available at Zenodo.


References

  1. 1.0 1.1 1.2 R. Rumpler, P. Göransson, J.-F. Deü. "A finite element approach combining a reduced-order system, Padé approximants, and an adaptive frequency windowing for fast multi-frequency solution of poro-acoustic problems", International Journal for Numerical Methods in Engineering, 97: 759-784, 2014.
  2. Q. Aumann, S. W. R. Werner. "Structured model order reduction for vibro-acoustic problems using interpolation and balancing methods", Journal of Sound and Vibration, 543: 117363, 2023.
  3. M. A. Biot. "Theory of propagation of elastic waves in a fluid-saturated porous solid. I. Low-frequency range", J. Acoust. Soc. Am., 28(2):168–178, 1956.