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Porous absorber: Difference between revisions

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Created page with "{{preliminary}} <!-- Do not remove --> ==Description== The '''Porous absorber''' benchmark models the sound pressure in a cavity excited by a single harmonic load. One side o..."
 
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{{preliminary}} <!-- Do not remove -->
{{preliminary}} <!-- Do not remove -->
<figure id="fig:plot1">
[[File:Porous_absorber.png|480px|thumb|right|<caption>Sketch of the geometry. The porous material is marked in blue, the acoustic source by <math>q</math>.</caption>]]
</figure>
<figure id="fig:tf">
[[File:Porous_absorber_frf.png|480px|thumb|right|<caption>Frequency response function.</caption>]]
</figure>


==Description==
==Description==

Revision as of 14:01, 27 June 2023

Note: This page has not been verified by our editors.

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].


References

  1. 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.