Experiments on reflection and transmission of acoustic porous metasurface with composite structure
Introduction
Sound isolation and absorption are important aspects in noise control and they are applied widely in architecture, ground transportation and even air transportation, e.g. roadside noise barriers, panels of car body and aircraft fuselage, etc. There is always a conflict between less sound transmission and less reflection, so that good sound absorption cannot be obtained. The dense materials with large acoustic impedance, e.g. metal and concrete, usually allow very little sound transmission. However, this kind of materials are heavy and reflect sound waves severely, which may cause secondary noise pollution. On the contrary, the materials with the impedance which can match with the air are able to cause less sound reflection, e.g. porous foam with high porosity, whereas they allow a large mount of sound transmission. It is a challenge to balance the reflection and transmission simultaneously to realize efficient noise control. It is expected that a composite structure or material is designed to reduce both the sound reflection and transmission to get good sound absorption performance.
In the current studies, there are many studies on the sound absorption performance and acoustic impedance of materials and composite structures [1], [2], [3], [4]. Thus, there arise a kind of artificially designed structures, so-called acoustic metamaterials [5], [6], which are carefully designed to obtain some uncommon acoustic properties that cannot be found in nature. Most acoustic metamaterials are studied based on passive control actions without external control load, however, there also arise some works about active control actions on elastic wave metamaterials [7]. In the current works on acoustic metamaterials for sound absorption, the focus of most attention is the material backed by a rigid wall [8], [9], [10], which is a common case for the applications of sound absorbers, e.g. sound absorption panel on the wall and acoustic liner in engine. In many cases, such as panels of car body and aircraft fuselage, the material is sandwiched by two plates for practical applications [11], [12]. Due to small thickness and elasticity of the plates, the sound will propagate through the structure and transmission is a necessary factor.
In addition to the acoustic performance, there are also some factors which should be considered in engineering applications, such as space limitation, corrosion and fire resistance etc. Under this background, a porous metasurface is designed in this work, resulting in less reflection and less transmission at the same time to obtain good sound absorption performance. The refracted behaviors and transmitted regularities of a periodic structure have been studied [13], while the reflected and transmitted phenomena will be considered at the same time during designing the composite structure in this work.
Section snippets
Conceptual design
When a sound wave incidents on a periodic structure and propagates through it, there are not only specular reflection and direct transmission. There occur additional reflected and refracted waves, which can be explained completely by the diffraction theory [14]. The diffraction theories for the reflection and refraction can be expressed as:where , and are the reflected, refracted and incident angles,
Analytical predictions and simulations on reflected and refracted behaviors
In this section, the reflected and the refracted behaviors are predicted analytically by the diffraction theory and validated by the numerical simulations. The simulation parts are implemented through solving the Helmhotz equation by a finite element solver COMSOL Multiphysics. The size of the maximum element is set as to guarantee the accuracy and convergence of the results. The incident wave is set as a plane wave at 2,000 Hz. The reflection region, metasurface domain and the refracted
Conclusion
An acoustic metasurface with composite structure is proposed for sound isolation and absorption considering both the reflection and transmission. It is a periodic structure containing four slits filled with a porous material in one period. The thicknesses of porous materials are designed to generate linear phase gradients for both the reflected and transmitted waves, which play key roles for the reflected and refracted phenomena. The regularities including the number of the reflected and the
Acknowledgement
Part of the study was supported by Hong Kong Innovation and Technology Commission (ITC) Project No. ITS/038/15FP. Yi Fang also wishes to thank Hong Kong University of Science and Technology for supporting part of Ph.D. thesis research.
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