Abstract:A strategy is developed for designing structures that radiate sound inefficiently in light fluids. The problem is broken into two steps. First, given a frequency and overall geometry of the structure, a surface velocity distribution is found that produces a minimum radiation condition. This particular velocity distribution is referred to as the "weak radiator" velocity profile. Second, a distribution of Young's modulus and density distribution is found for the structure such that it exhibits the weak radiator … Show more
“…In that example, the "rst eigenfrequency of an engine cover plate was decreased while the radiated noise level was reduced by about 12 dB. Similar investigations [17] were reported for piecewise constant material data like Young's modulus or density. Reductions between 2 and 23 dB were achieved.…”
“…In that example, the "rst eigenfrequency of an engine cover plate was decreased while the radiated noise level was reduced by about 12 dB. Similar investigations [17] were reported for piecewise constant material data like Young's modulus or density. Reductions between 2 and 23 dB were achieved.…”
“…Shape optimization has been shown to be effective by Bernard (1985) and Wilcox and Lalor (1987). More recent work in this area has been carried out by Lamancusa (1988), Sivakumar et al (1991) and Naghshineh et al (1992).…”
A general approach for minimizing radiated acoustic power of a baffled plate excited by broad band harmonic excitation is given. The steps involve a finite element discretization for expressing acoustic power and vibration analysis, analytical design sensitivity analysis, and the use of gradient-based optimization algorithms. Acoustic power expressions arc derived from the Rayleigh integral for plates. A general methodology is developcd for computing design sensitivities using analytical expressions. Results show that analytical scnsitivity analysis is important from both computational time and accuracy considerations. Applications of the optimization strategy to rcctangular plates and an engine cover plate are prcscnted. Thicknesscs are chosen as design variables.
“…An alternative to this would be to calculate the optimum modal weight vector from a purely acoustic optimisation procedure, as described by Naghshineh et al in Ref. [14] and then try to adjust the structural parameters in order to obtain the desired modal weight vector. However, one of the problems with this approach is that matching the calculated modal weight vector with the desired modal weight vector cannot be achieved perfectly under all constraint mass and stiffener conditions.…”
Section: Optimisation To Achieve Weak Acoustical Radiationmentioning
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