Microstructures for lowering the quarter wavelength resonance frequency of a hard-backed rigid-porous layer

The frequency of the quarter wavelength resonance in the sound absorption spectra due to a thin hard-backed rigid-porous layer can be influenced by the design of its microstructure as well as its thickness. Microstructures considered include parallel arrays of identical cylindrical, slit-like or rectangular pores with deep sub-wavelength cross sections inclined to the surface normal, cylindrical annular pores, slits with log-normal width distributions, slits with cross sections that vary in a sinusoidal manner and slits with two distinct widths (dual porosity). Formulae that predict the bulk acoustical properties due to these microstructures are presented and used to explore the extent to which specific microstructures could be used separately or in combination to improve low-frequency absorption. Predicted normal incidence absorption coefficient spectra are compared using microstructural dimensions that would be feasible for 3D printing. The most effective microstructures are predicted to be slits with sinusoidally-varying widths, or with two distinct widths, inclined to the surface normal at 70°. The quarter wavelength layer resonances predicted in absorption coefficient spectra using these microstructures are comparable with those predicted for layers of the same thickness and bulk porosity having cylindrical pores with dead-end branches.

[1]  Yvan Champoux,et al.  On acoustical models for sound propagation in rigid frame porous materials and the influence of shape factors , 1992 .

[2]  T. Lu,et al.  Modeling of roughness effects on acoustic properties of micro-slits , 2017 .

[3]  Tokuo Yamamoto,et al.  Acoustic wave propagation through porous media with arbitrary pore‐size distributions , 1987 .

[4]  Joel Koplik,et al.  Theory of dynamic permeability and tortuosity in fluid-saturated porous media , 1987, Journal of Fluid Mechanics.

[5]  Simon N. Chandler-Wilde,et al.  Padé approximants for the acoustical properties of rigid frame porous media with pore size distributions , 1998 .

[6]  Denis Lafarge,et al.  Dynamic compressibility of air in porous structures at audible frequencies , 1997 .

[7]  Yvan Champoux,et al.  Propagation of sound and the assignment of shape factors in model porous materials having simple pore geometries , 1992 .

[8]  Olivier Dazel,et al.  Asymptotic limits of some models for sound propagation in porous media and the assignment of the pore characteristic lengths. , 2016, The Journal of the Acoustical Society of America.

[9]  R. Venegas,et al.  Sound propagation in porous materials with annular pores. , 2017, The Journal of the Acoustical Society of America.

[10]  K V Horoshenkov,et al.  The acoustic properties of granular materials with pore size distribution close to log-normal. , 2001, The Journal of the Acoustical Society of America.

[11]  P Leclaire,et al.  Acoustical properties of air-saturated porous material with periodically distributed dead-end pores. , 2015, The Journal of the Acoustical Society of America.

[12]  P. Carman,et al.  Flow of gases through porous media , 1956 .

[13]  Ren Shu-wei,et al.  Sound Absorption Enhancement by Thin Multi-Slit Hybrid Structures , 2015 .

[14]  M. R. Stinson The propagation of plane sound waves in narrow and wide circular tubes, and generalization to uniform tubes of arbitrary cross- sectional shape , 1991 .

[15]  Microstructure based model for sound absorption predictions of perforated closed-cell metallic foams. , 2010, The Journal of the Acoustical Society of America.

[16]  David A. Harris,et al.  Sound Absorbing Materials , 1991 .

[17]  Claude Boutin,et al.  Acoustic wave propagation in double porosity media. , 2003, The Journal of the Acoustical Society of America.