Part I of this paper has shown the suitability of wavenumber}frequency approach in the calculation of the vibro-acoustic response of a thin ba%ed plate to a large class of random excitations. Part II describes the application of this formulation to the prediction of the vibration and the acoustic ra
A WAVENUMBER APPROACH TO MODELLING THE RESPONSE OF A RANDOMLY EXCITED PANEL, PART I: GENERAL THEORY
β Scribed by C. MAURY; P. GARDONIO; S.J. ELLIOTT
- Publisher
- Elsevier Science
- Year
- 2002
- Tongue
- English
- Weight
- 360 KB
- Volume
- 252
- Category
- Article
- ISSN
- 0022-460X
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β¦ Synopsis
Part I of this paper presents a self-contained analytical framework for determining the vibro-acoustic response of a plate to a large class of random excitations. The wavenumber approach is used, which provides an insight into the physical properties of the panel response and enables us to evaluate e$ciently the validity of several simplifying assumptions. This formulation is used in Part II for predicting the statistical response of an aircraft panel excited by a turbulent boundary layer. In this paper, we "rst provide a general statement of the problem and describe how the spectral densities of the panel response can be obtained from an analysis of the system response to a harmonic deterministic excitation and a statistical model for the forcing "eld. The harmonic response of the system is then expanded as a series of the eigenmodes of the #uid-loaded panel and these #uid-loaded eigenmodes are approximated by a perturbation method. Then, we evaluate the conditions under which this series simpli"es into a classical modal formulation in terms of the in vacuo eigenmodes.
To illustrate the use of a wavenumber approach, we consider three examples, namely, the vibro-acoustic response of a panel excited by an incidence di!use acoustic "eld, by a fully developed turbulent #ow and by a pressure "eld which is spatially uncorrelated from one point to another. Convergence properties of the modal formulations are also examined.
2002 Elsevier Science Ltd. C. MAURY EΒΉ AΒΈ. where L . (w)"D *w *x # *w *y !N V *w *x !N W *w *y , ! 1 c $ * *t p $ (z; t)"0, z3 $ , (4) $ *w *t (x; t)# *p $ *z (x; t)"0, x3 , (5) *p $ *z (x; t)"0, x3 , (6) w(x; 0)" *w *t (x; 0)"0, x3 , (7)
π SIMILAR VOLUMES
In a previous series of papers [1][2][3], a general model based on Hamilton's
## Abstract A Monte Carlo method is presented to calculate equilibria for the binding of ligands to oneβdimensional heteropolymers. Equivalency with other methods suitable for particular cases was verified (i.e., matrix and combinatorial methods). The principal interest of this Monte Carlo method i
Use of the higher order method of multiple scales with reconstitution to determine the periodic steady state response of harmonically excited non-linear oscillators is considered. The well known primary resonance in the Duffing oscillator is considered as a prototype example. Second order mutliple-s