2018
DOI: 10.1002/mana.201700489
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Stability analysis of coupled structural acoustics PDE models under thermal effects and with no additional dissipation

Abstract: In this study we consider a coupled system of partial differential equations (PDE's) which describes a certain structural acoustics interaction. One component of this PDE system is a wave equation, which serves to model the interior acoustic wave medium within a given three dimensional chamber Ω. This acoustic wave equation is coupled on a boundary interface Γ 0 to a two dimensional system of thermoelasticity: this thermoelastic PDE is composed in part of a structural beam or plate equation, which governs the … Show more

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Cited by 10 publications
(7 citation statements)
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“…For some recent work on the mathematical analysis of acoustics-structure interaction problems we refer to, e.g., [1,2,3,34,35] and the references therein. Most of these models involve a linear or semi-linear wave equation coupled with linear and nonlinear plate models.…”
Section: Introductionmentioning
confidence: 99%
“…For some recent work on the mathematical analysis of acoustics-structure interaction problems we refer to, e.g., [1,2,3,34,35] and the references therein. Most of these models involve a linear or semi-linear wave equation coupled with linear and nonlinear plate models.…”
Section: Introductionmentioning
confidence: 99%
“…In view of relation (13), we should strive to majorize solution Φ of (10) in norm in terms of the static heat dissipation. With this theme in mind, from the mechanical compatibility conditions in (5), and the resolvent relations and matching velocity BC's in (11), we have for j = 1, ..., K,…”
Section: Proof Of Theoremmentioning
confidence: 99%
“…(In our future work on discerning uniform decay properties of solutions to the multilayered FSI system (2)-( 5), the spectral information in Theorem 2 is also requisite; see e.g., the resolvent criteria in [27] and [12].) In showing the nonpresence of σ(A) on the imaginary axis -in particular, to handle the continuous spectrum of Awe will proceed in a manner somewhat analogous to what was undertaken in [7] (in which another coupled PDE system, with the coupling accomplished across a boundary interface, is analyzed with a view towards stability). However, the thin layer wave equation in (3) again gives rise to complications: In the course of eliminating the possibility of approximate spectrum of A on iR, we find it necessary to invoke the wave multipliers which are used in PDE control theory for uniform stabilization of boundary controlled waves: namely, inasmuch as each h j -wave equation in (3) carries the difference of the 3-D wave and heat fluxes as a forcing term, we cannot immediately control the thick wave trace ∂w ∂ν Γs in H − 1 2 (Γ s )norm, this control being needed for strong decay.…”
Section: Novelty and Challengesmentioning
confidence: 99%