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Pneumatically-Actuated Acoustic Metamaterials Based on Helmholtz Resonators

机译:基于Helmholtz谐振器的气动驱动声学超材料

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摘要

Metamaterials are periodic structures which offer physical properties not found in nature. Particularly, acoustic metamaterials can manipulate sound and elastic waves both spatially and spectrally in unpreceded ways. Acoustic metamaterials can generate arbitrary acoustic bandgaps by scattering sound waves, which is a superior property for insulation properties. In this study, one dimension of the resonators (depth of cavity) was altered by means of a pneumatic actuation system. To this end, metamaterial slabs were additively manufactured and connected to a proportional pressure control unit. The noise reduction performance of active acoustic metamaterials in closed- and open-space configurations was measured in different control conditions. The pneumatic actuation system was used to vary the pressure behind pistons inside each cell of the metamaterial, and as a result to vary the cavity depth of each unit cell. Two pressures were considered, P = 0.05 bar, which led to higher depth of the cavities, and P = 0.15 bar, which resulted in lower depth of cavities. The results showed that by changing the pressure from P = 0.05 (high cavity depth) to P = 0.15 (low cavity depth), the acoustic bandgap can be shifted from a frequency band of 150–350 Hz to a frequency band of 300–600 Hz. The pneumatically-actuated acoustical metamaterial gave a peak attenuation of 20 dB (at 500 Hz) in the closed system and 15 dB (at 500 Hz) in the open system. A step forward would be to tune different unit cells of the metamaterial with different pressure levels (and therefore different cavity depths) in order to target a broader range of frequencies.
机译:超材料是周期性结构,提供本质上未发现的物理性质。特别地,声学的超材料可以以前所未有的方式在空间和光谱上操纵声音和弹性波。声学超材料可以通过散射声波产生任意声学带隙,这是绝缘性能的优越性。在该研究中,通过气动致动系统改变谐振器的一个尺寸(空腔深度)。为此,超材料板被加容量制造并连接到比例压力控制单元。在不同的控制条件下测量了闭合空间配置中有源声学超材料的降噪性能。气动致动系统用于改变超材料的每个电池内的活塞后面的压力,结果改变每个单元电池的腔深度。考虑了两个压力,P = 0.05巴,其导致腔的深度较高,P = 0.15巴,导致腔的较低深度。结果表明,通过将来自P = 0.05(高腔深度)的压力改变为P = 0.15(低腔深),声学带隙可以从150-350 Hz的频带移位到300-600的频带赫兹。气动驱动的声学超材料在封闭系统中达到20dB(处为500Hz)的峰值衰减,在开放系统中为15dB(在500Hz处)。前进的一步是用不同的压力水平(因此不同的腔深)调谐超材料的不同单元电池,以便瞄准更宽范围的频率。

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