A Validated Finite Element Model for Room Acoustic Treatments with Edge Absorbers

TL;DR

This paper presents a validated finite element model capable of accurately simulating the effects of edge absorbers on room acoustics, addressing limitations of traditional geometrical methods at low frequencies.

Contribution

A novel finite element simulation model for edge absorbers is developed and validated, enabling detailed analysis of low-frequency acoustic interactions in rooms.

Findings

Finite element model predicts transfer functions with 3.25-4.11dB accuracy.

Model effectively visualizes interaction mechanisms between room and absorber.

Validated against experimental data in a reverberation chamber.

Abstract

Porous acoustic absorbers have excellent properties in the low-frequency range when positioned in room edges, therefore they are a common method for reducing low-frequency reverberation. However, standard room acoustic simulation methods such as ray tracing and mirror sources are invalid for low frequencies in general which is a consequence of using geometrical methods, yielding a lack of simulation tools for these so-called edge absorbers. In this article, a validated finite element simulation model is presented, which is able to predict the effect of an edge absorber on the acoustic field. With this model, the interaction mechanisms between room and absorber can be studied by high-resolved acoustic field visualizations in both room and absorber. The finite element model is validated against transfer function data computed from impulse response measurements in a reverberation chamber in style of ISO 354. The absorber made of Basotect is modeled using the Johnson-Champoux-Allard-Lafarge model, which is fitted to impedance tube measurements using the four-microphone transfer matrix method. It is shown that the finite element simulation model is able to predict the influence of different edge absorber configurations on the measured transfer functions to a high degree of accuracy. The evaluated third-octave band error exhibits deviations of 3.25dB to 4.11dB computed from third-octave band averaged spectra.