2011
DOI: 10.1016/j.jsv.2011.05.029
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Numerical investigation of active porous composites with enhanced acoustic absorption

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Cited by 22 publications
(15 citation statements)
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“…at 0.9 kHz and 1.8 kHz) acoustic resonances resulting from the motion of elastic skeleton of the soft PU foam are visible; at higher frequencies the skeleton behaviour tends to be rigid even for the soft PU foam. This is a typical situation for soft PU foams: the low-frequency resonances and anti-resonances of elastic skeleton significantly influence sound propagation and absorption; the flexibility of elastic skeleton may also be utilized in order to improve the acoustic absorption in semi-active (Zielinski, Rak, 2010) or active way (Zielinski, 2008;2010;2011). The sound absorption properties of PU foams may also be improved passively by changing the skeleton density and stiffness -this can be attained by adding some inclusions in the foam matrix, for example, rice hull (Wang et al, 2013), or tea-leaf-fibres (Ekici, 2012).…”
Section: Discussion Of the Resultsmentioning
confidence: 99%
“…at 0.9 kHz and 1.8 kHz) acoustic resonances resulting from the motion of elastic skeleton of the soft PU foam are visible; at higher frequencies the skeleton behaviour tends to be rigid even for the soft PU foam. This is a typical situation for soft PU foams: the low-frequency resonances and anti-resonances of elastic skeleton significantly influence sound propagation and absorption; the flexibility of elastic skeleton may also be utilized in order to improve the acoustic absorption in semi-active (Zielinski, Rak, 2010) or active way (Zielinski, 2008;2010;2011). The sound absorption properties of PU foams may also be improved passively by changing the skeleton density and stiffness -this can be attained by adding some inclusions in the foam matrix, for example, rice hull (Wang et al, 2013), or tea-leaf-fibres (Ekici, 2012).…”
Section: Discussion Of the Resultsmentioning
confidence: 99%
“…II A. Whatever the case, when the surface acoustic impedance of a two-layered (17) or single-layer medium (18) is known, the complex-valued reflection coefficient R and the real-valued acoustic absorption coefficient A can be calculated 12,16 as…”
Section: Modeling the Acoustic Impedance And Absorption Of Porousmentioning
confidence: 99%
“…The poroelastic model for sound absorbing media must be used when the vibrations of the solid frame cannot be neglected, for example, in the case of soft porous media or in active systems involving porous materials. [14][15][16] The essential parameters of the Johnson-Allard (JCA, JCAL, or JCAPL) and Biot-Allard models which result from the micro-geometry of the solid frame are in fact some sort of macroscopic, average geometric characteristics of the porous medium derived on the basis of homogenization theory. Although, they can be measured directly (see, for example, Refs.…”
Section: Introductionmentioning
confidence: 99%
“…Basing on the results of surface acoustic impedance the acoustic absorption coefficient AðxÞ was computed using the following formulas: 21,40 A…”
Section: Surface Acoustic Impedance and Absorption For Rigid Foam mentioning
confidence: 99%