SmEdA vibro-acoustic modelling in the mid-frequency range including the effect of dissipative treatments. (14th April 2017)

• Record Type: Journal Article
• Authors: Hwang, H.D.; Maxit, L.; Ege, K.; Gerges, Y.; Guyader, J.-L.
• Is Part Of: Journal of sound and vibration. Volume 393(2017)
• Page Start: 187
• Page End: 215
• Publication Date: 2017-04-14
• Subjects: Vibro-acoustic modelling -- Fluid-structure interaction -- Mid-frequency analysis -- Viscoelastic layer -- Porous materials -- Modal damping loss factor; Sound -- Periodicals; Vibration -- Periodicals; Son -- Périodiques; Vibration -- Périodiques; Sound; Vibration; Periodicals; Electronic journals; 620.205
• DOI: 10.1016/j.jsv.2017.01.024
• Languages: English
• ISSNs: 0022-460X

Abstract

Abstract: Vibro-acoustic simulation in the mid-frequency range is of interest for automotive and truck constructors. The dissipative treatments used for noise and vibration control such as viscoelastic patches and acoustic absorbing materials must be taken into account in the problem. The Statistical modal Energy distribution Analysis (SmEdA) model consists in extending Statistical Energy Analysis (SEA) to the mid-frequency range by establishing power balance equations between the modes of the different subsystems. The modal basis of uncoupled-subsystems that can be estimated by the finite element method in the mid-frequency range is used as input data. SmEdA was originally developed by considering constant modal damping factors for each subsystem. However, this means that it cannot describe the local distribution of dissipative materials. To overcome this issue, a methodology is proposed here to take into account the effect of these materials. This methodology is based on the finite element models of the subsystems that include well-known homogenized material models of dissipative treatments. The Galerkin method with subsystem normal modes is used to estimate the modal damping loss factors. Cross-modal coupling terms which appear in the formulation due to the dissipative materials are assumed to be negligible. An approximation of the energy sharing between the subsystems damped by dissipative materials is then described by SmEdA. The different steps of the method are validated experimentally by applying it to a laboratory test case composed of a plate-cavity system with different configurations of dissipative treatments. The comparison between the experimental and the simulation results shows good agreement in the mid-frequency range.