Abstract

When predicting the radiation of structure-borne sound into a room, it is often assumed that the generated sound field is diffuse. A diffuse field is by definition a random field, composed of a large number of statistically independent plane waves, the spatial phase of which is uniformly distributed and independent from the amplitude. It may represent the sound field of a conceptual ensemble of rooms with the same modal density and total absorption, but otherwise any possible arrangement of boundaries and small objects that scatter incoming sound waves. Adopting a diffuse field model therefore inherently implies that uncertainty due to random wave scattering is present in the computed results. This uncertainty can be large, especially at low frequencies. In this work, practical formulas are derived for computing not only the mean, but also the variance of energetic level quantities, such as the band-integrated spatially averaged sound pressure level, in a diffuse sound field caused by a mechanically excited structure. The obtained expressions are first verified in a simulation study, and then experimentally validated for a point-loaded bare plate and a rib-stiffened plate. It is found that both the average sound pressure level and its standard deviation can be well predicted. Knowledge of this standard deviation then allows the analyst to estimate, for example, by how much the spatially averaged sound pressure level in one particular room can deviate from the ensemble averaged result, and this for any frequency band.

Highlights

  • In a noise control context, structure-borne sound refers to sound that is generated by direct mechanical excitation of a structure, such as a building, a car body or an aircraft fuselage [1]

  • It can be verified that all of the previous expressions involving sound power remain valid for non-periodic stationary excitation, but the power quantities involved need be re-defined as power spectral densities, e.g., Win need be expressed in Watt per Hertz (W∕Hz) rather than Watt (W)

  • It has been assumed that the vibration field of the radiating structure depends on the direct mechanical excitation and possibly on energy that is radiated into the direct sound field, but not on the diffuse sound pressure field, such that the vibration field can be computed independently from the total energy of the diffuse sound field

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Summary

Introduction

In a noise control context, structure-borne sound refers to sound that is generated by direct mechanical excitation of a structure, such as (a part of) a building, a car body or an aircraft fuselage [1]. The uncertainty that is inherent in the diffuse field model is larger because of the lower modal overlap This implies that considerable variation can occur when comparing the mean total sound energy of a diffuse room model with the total sound energy for one particular member of the random ensemble.

Predicting the vibration field of the radiating structure
General expressions
Spatially averaged mean sound pressure
Generalization to stationary excitation
Variance and probability distribution of the sound pressure
Energetic weighting and integration in frequency bands
Mean and variance of level quantities
Numerical verification
Experimental case studies
Bare PMMA panel
Rib-stiffened PMMA panel
Concluding remarks
Full Text
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