Abstract

In many different fields of engineering, like automotive industry or civil engi- neering, room acoustical tasks are of interest. Sound fields have to be predicted in order to design the acoustic cavity by placing acoustic elements like reflectors or absorbers (passive absorbers or plate resonators) into the room for example. Therefore models for the Fluid Structure Interaction (FSI) are used, where passive absorbers or plate resonators can be con- sidered. For simulations of the spatial resolution of the sound field within acoustic cavities very often techniques based on Finite Element formulations are used. In order to reduce the number of degrees of freedom and therefore the numerical effort, a model reduction method, based on a Component Mode Synthesis (CMS), is applied in this contribution. The advan- tage is related to the fact, that the modal analysis is done only once for the rigid walled cavity, which is modeled with Spectral Finite Elements (SFEM). The cavity boundary condi- tions, e.g. compound absorbers made of homogenous plates and porous foams, are modeled using Integral Transform Methods (ITM). Therefore the differential equations of motion are established for the individual components, where the Lam´ e Equation is used for homogenous and the Theory of Porous Media (TPM) for porous materials. These equations are solved in the wavenumber-frequency domain after applying a Fourier Transformation. The results (wavenumber dependent impedances) for the absorptive structure are coupled with the acous- tic cavity adding interface coupling modes for the fluid and applying Hamilton's principle, considering the velocity of both components to coincide as a constraint at the interface. The method is presented and models of the subsystems, the absorber and the fluid, are shown. Finally examples for the simulation of the coupled structure are presented.

Highlights

  • Due to increasing requirements of comfort, acoustic design has become more important during the last years, especially in the field of civil engineering and automotive design.The sound field within rooms or vehicles has to be predicted and modified in an acoustic optimization process in order to reach an optimal result for the specific use.The calculation of the sound pressure level inside of acoustic cavities is usually done with the help of the Statistical Energy Analysis (SEA)

  • The application of the Component Mode Synthesis (CMS) approach provides the possibility to recalculate the system for small changes in geometry or load data with low numerical effort

  • The normal and constraint modes for the acoustic cavity are calculated with the Spectral Finite Elements (SFEM)

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Summary

INTRODUCTION

Due to increasing requirements of comfort, acoustic design has become more important during the last years, especially in the field of civil engineering and automotive design. The calculation of the sound pressure level inside of acoustic cavities is usually done with the help of the Statistical Energy Analysis (SEA) This method is robust for systems with a high modal density and it is based on an averaging over frequency bands, points of excitation and points of observation. A robust method for the phase correct modeling of interior sound fields with sufficient spatial resolution is needed, where the absorptive behavior of the delimiting surfaces can be considered. Methods, based on Finite Element formulations are used for this purpose, where the robustness can be enhanced by applying an averaging in the post-processing. This requires multiple calculations with slight changes in geometry or load data [5]. Especially to reduce the computational effort for the optimization of the position of these acoustic elements or for averaging techniques as mentioned above, is to simulate the coupled system (fluid-structure) in the frequency domain by applying a CMS

FLUID STRUCTURE INTERACTION
Hamiltons Principle and Ritz Approach
Component mode Synthesis
COMPOUND ABSORBERS
Classification
Material Description
Boundary Conditions and Equation System
COUPLING THE SUBSYSTEMS AND ASSEMBLING THE EQUATION SYSTEM
Application to a 1d Structure
Application to a 2d Structure
CONCLUSION
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