Abstract

A diffuse sound field is conventionally defined as a zero-mean circularly symmetric complex Gaussian random field. A more recent, generalized definition is that of a sound field having mode shapes that are diffuse in the conventional sense, and eigenfrequencies that conform to the Gaussian orthogonal ensemble. Such a generalized diffuse sound field can represent a random ensemble of sound fields that share gross features, such as modal density and total absorption, but otherwise have any possible arrangement of local wave scattering features. The problem of generating realizations or Monte Carlo samples of a conventional diffuse sound field or, equivalently, of the mode shapes of a generalized diffuse sound field, is addressed here. Such realizations can be obtained from an eigenvalue decomposition of the spatial correlation function. A discrete decomposition is numerically expensive when the sound pressures at many locations are of interest, so a fast analytical decomposition based on prolate spheroidal wave functions is developed. The approach is numerically validated by comparison with a detailed room model, where random wave scatterers are explicitly modeled as acoustic point masses with random positions, and good correspondence is observed. Furthermore, applications involving correlated sound sources and sound-structure interaction are presented.

Highlights

  • INTRODUCTIONIf the acoustic wavelength is small compared to the characteristic size (e.g., the mean free path) of an enclosed space, the sound field in that space is often modeled as diffuse

  • If the acoustic wavelength is small compared to the characteristic size of an enclosed space, the sound field in that space is often modeled as diffuse

  • Such a generalized diffuse sound field can represent a random ensemble of sound fields that share gross features, such as modal density and total absorption, but otherwise have any possible arrangement of local wave scattering features

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Summary

INTRODUCTION

If the acoustic wavelength is small compared to the characteristic size (e.g., the mean free path) of an enclosed space, the sound field in that space is often modeled as diffuse. Field is generated by an enclosure that has mode shapes that are diffuse in the conventional sense, and a squared eigenfrequency spacings distribution that conforms to the Gaussian orthogonal ensemble (GOE) eigenvalue spacings distribution.4,5 This generalized diffuse field model is known to be valid for all vibro-acoustic systems for which the uncertainty of the local field quantity, due to the small random wave scattering elements, is large.. The PSWF theory is invoked for obtaining the Karhunen–Loeve decomposition of the spatial correlation function, such that Monte Carlo samples of the diffuse sound pressures at a large number of locations can be efficiently generated. The approach is validated in applications where the sound field needs to be evaluated at many locations, such as the evaluation of the sound field in a room with a loudspeaker array or the interaction between a sound field and a vibrating surface

Pressure distribution in a diffuse sound field
Karhunen–Loeve decomposition
DIFFUSE PRESSURE FIELD ON A LINE
Eigenfunctions from angular prolate spheroidal wave functions
Eigenvalues from radial prolate spheroidal wave functions
Generation of diffuse pressure fields
Theory
À k2 ÀDy2
Application
A GENERALIZED DIFFUSE SOUND FIELD
Generation of natural frequencies in a diffuse field
Generation of modeshapes in a diffuse field
Application 1
Application 2
Application 3
CONCLUSIONS
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