Effect of Air Gap, Thickness of Polyurethane (PU) Foam, and Perforated Panel on Sound Absorption Coefficient for Acoustic Structures

Chetan Patil, Ratnakar R. Ghorpade, R. Askhedkar
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Abstract

There are many applications and sectors in today’s era where noise pollution is reaching very high levels. This prolonged noise exposure leads to a detrimental health effect. This may cause loss of concentration, working efficiency, headache, increased blood pressure level, annoyance, and even workplace accidents. Hence, the need to reduce the high noise level is becoming a significant issue. Varieties of absorbing materials are being used in the recent age for noise reduction and sound attenuation. Most of the acoustic enclosures consist of polyurethane foam as a sound absorber. The noise control is achieved by modifying the noise source characteristics, path modification, or muffling at the receiver. The best way to control noise is noise absorption, where acoustic materials are designed to absorb sound. Polyurethane foam is widely accepted because of its good properties like wide absorption frequency range, structural stabilization, low cost, easy handling, and moisture resistance. It has been observed that the sound absorption coefficient (SAC) depends on the thickness of polyurethane foam and the air gap. This paper discusses the different acoustic properties of various acoustic structures consisting of the perforated panel, air gap, and polyurethane foam for the frequency range of 100–4000 Hz. Different combinations of acoustic structures are proposed to observe the effect of absorptivity in terms of sound attenuation. The effect of layer sequence on the acoustic absorption of the structure has been investigated. The relation between the thickness of the material, air gap, and SAC are also analyzed. FEA can accurately analyze the absorption characteristics at normal incidence of sound-absorbing structure. The acoustic structure consisting of polyurethane foam gives the maximum value of SAC for a frequency range of 2300–4000 Hz. The acoustic structure consisting of the perforated panel, air gap, and polyurethane foam give the maximum SAC value for the lower frequency range of 100 to 2300 Hz. In the current study, it has been seen that the acoustic structure consisting of polyurethane foam with an air gap gives the minimum value of SAC. The SAC varies with the air gap and thickness of the foam. The study affirmed that using the perforated panels in acoustic structure gives the maximum value of SAC in the lower frequency range. The SAC of a material is calculated with an analytical method and verified with the experimental method and FEA software. For verification of SAC for different acoustic structures, COMSOL Multiphysics 5.5 results are seen to be in good agreement with a maximum difference of 8.1% with that of the experimental results.
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气隙、聚氨酯(PU)泡沫厚度和穿孔板对声学结构吸声系数的影响
在当今时代,有许多应用和部门的噪音污染达到了非常高的水平。长时间接触噪音对健康有害。这可能会导致注意力不集中、工作效率低下、头痛、血压升高、烦恼,甚至发生工作事故。因此,降低高噪声水平的需要成为一个重要的问题。近年来,各种各样的吸声材料被用于降噪和消声。大多数隔音罩由聚氨酯泡沫作为吸声材料组成。噪声控制是通过修改噪声源特性、路径修改或接收机消声来实现的。控制噪音的最好方法是吸声,即设计隔音材料来吸收声音。聚氨酯泡沫因其吸收频率范围宽、结构稳定、成本低、易处理、防潮等优良性能而被广泛接受。研究发现,吸声系数与聚氨酯泡沫材料的厚度和气隙有关。本文讨论了由多孔板、气隙和聚氨酯泡沫组成的不同声学结构在100-4000 Hz频率范围内的声学性能差异。提出了不同的声结构组合来观察吸声率对声衰减的影响。研究了层序对结构吸声性能的影响。分析了材料厚度、气隙和SAC之间的关系。有限元分析可以准确地分析吸声结构法向入射处的吸声特性。由聚氨酯泡沫组成的声学结构在2300-4000 Hz的频率范围内给出了SAC的最大值。由穿孔板、气隙和聚氨酯泡沫组成的声学结构在100至2300 Hz的较低频率范围内给出了最大的SAC值。在目前的研究中,已经看到由带有气隙的聚氨酯泡沫组成的声学结构具有最小的SAC值。SAC随泡沫的气隙和厚度而变化。研究证实,在声学结构中使用穿孔板,在低频范围内SAC值最大。用分析方法计算了材料的SAC,并用实验方法和有限元软件进行了验证。为了验证不同声学结构的SAC, COMSOL Multiphysics 5.5的结果与实验结果的最大差异为8.1%,符合得很好。
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