
materials Article Pneumatically-Actuated Acoustic Metamaterials Based on Helmholtz Resonators Reza Hedayati * and Sandhya Lakshmanan Novel Aerospace Materials group, Faculty of Aerospace Engineering, Delft University of Technology (TU Delft), Kluyverweg 1, 2629 HS Delft, The Netherlands; [email protected] * Correspondence: [email protected] or [email protected] Received: 24 February 2020; Accepted: 19 March 2020; Published: 23 March 2020 Abstract: 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. Keywords: active noise control; acoustic metamaterial; broadband noise attenuation; pneumatic actuation; Helmholtz resonators 1. Introduction Metamaterials are periodic designer materials which offer physical properties not found in nature [1]. Particularly, acoustic metamaterials can manipulate sound and elastic waves both spatially and spectrally in unpreceded ways [2]. Such properties include super-focusing [3], super-lensing [4], active membrane structures [5,6], cloaking [7,8], phononic plates [9], fluid cavities separated by piezoelectric boundaries [10], and tunable noise attenuation based on Helmholtz resonators [11–15]. The capability of metamaterials to tune their physical behavior just based on their geometrical characteristics offers a great benefit over conventional materials for application in various high-demand industries such as aerospace, automobile, and construction. Increase in importance of customer comfort in transportation and construction sectors as well as consumer goods has been a driving force for recent advancements in acoustic metamaterials in the field of noise control. Acoustic metamaterials can generate arbitrary acoustic bandgaps by scattering sound waves, which is a superior property for insulation properties. Initially, the acoustic metamaterials were passive; their performance remained unchanged and it was in accordance to the design values [16–18]. More recently, the concept of tunable acoustic Materials 2020, 13, 1456; doi:10.3390/ma13061456 www.mdpi.com/journal/materials Materials 2020, 13, 1456 2 of 11 Materialsmetamaterials 2020, 13, x FOR has PEER emerged REVIEW in which acoustic metamaterials are able to manipulate sound2 waves of 11 in various conditions [6–8,19–21]. Active acoustic metamaterials can be responsive to different stimuli, varioussuch conditions as electric [6–8,19–21]. field [21], electromagnetic Active acoustic field meta [6,materials22], mechanical can be loadresponsive [11], and to electricitydifferent stimuli, by means of suchpiezoelectric as electric field elements [21], electromagnetic [7]. field [6,22], mechanical load [11], and electricity by means of piezoelectricAcoustic elements metamaterials [7]. are widely preferred in applications where high efficiency in noise reductionAcoustic metamaterials is expected. As are an widely important preferred design in parameter applications in this where regard high is simplicityefficiency inin designnoise yet reductionbeing is eff expected.ective in performance, As an important Helmholtz design resonance parameter provides in this regard a lucrative is simplicity solution (Figurein design1). yet Due to beingits effective simplistic in geometricalperformance, characteristics, Helmholtz resonance Helmholtz provides resonators a lucrative have been solution incorporated (Figure 1). into Due acoustic to its simplisticmetamaterials. geometrical The Helmholtz characteristics, resonator Helmholtz is a phenomenon resonators where have been acoustic incorporated resonance into is created acoustic when a metamaterials.gas (typically The air) Helmholtz passes over resonator the opening is a phenom (also calledenon neck) where of acoustic an enclosed resonance cavity. is The created system when working a gasresembles (typically that air) of passes a mass-spring over the system.opening The (als airo called inside neck) the cavity of an works enclosed as a springcavity. andThe the system air in the workingneck resembles works as athat mass. of a When mass-s anpring incoming system. air The pressure air inside acts the upon cavity the airworks occupying as a spring the neckand the region, air init the pushes neck itworks down as into a mass. the cavity. When Hence,an incoming the air air inside pressure the cavity acts upon becomes the air compressed occupying andthe neck attempts region,to retainit pushes its originalit down volume.into the cavity. This pushes Hence, back the theair inside air inside the thecavity neck becomes and creates compressed a counteracting and attemptsacoustic to retain resonance its original with respect volume. to the This initial pu incomingshes back acousticthe air wave.inside Whenthe neck the airand pressure creates insidea counteractingthe cavity acoustic decreases, resonance it sucks airwith around respect the to neck the area initial back incoming again, and acoustic this phenomenon wave. When repeats the air itself pressureseveral inside times the making cavity the decreases, air inside theit sucks cavity workair around similar the to aneck spring. area In recentback years,again, thereand hasthis been phenomenonextensive repeats research itself in development several times of making acoustic the metamaterials air inside the constructedcavity work fromsimilar Helmholtz to a spring. resonator In recentunit years, cells there [13–15 has] to been generate extensive tunable research band in gaps. development of acoustic metamaterials constructed from HelmholtzThe Helmholtz resonator resonator unit cells equation [13–15] isto [generate23] tunable band gaps. The Helmholtz resonator equation is [23] r c A f = (1) = 2π VL (1) where c is the speed of sound in the medium (i.e., air), L is the neck length, A is the neck cross-sectional wherearea, is and theV speedis the of volume sound ofin mediumthe medium in the (i.e., cavity. air), As is it the can neck be deduced length, from is the Equation neck cross- (1), three sectionalgeometrical area, and characteristics is the volume (cross-sectional of medium in area theA cavity.and length As it canL of be neck deduced as well from as theEquation volume (1), of the threecavity geometricalV) can becharacteristics actively altered (cross-sectional to produce tunabilityarea and in length the performance of neck ofas metamaterial.well as the volume The most of theconvenient cavity ) can way be to actively actively altered adjust to the produce performance tunability of metamaterialin the performance is tuning of metamaterial. the cavity volume The as mostthe convenient actuation way system to actively would adjust not need the toperforma performnce in of the metamaterial vicinity of the is tuning neck where the cavity the metamaterial volume as theinteracts actuation the system most with would incoming not need external to perform sound in pressures.the vicinity of the neck where the metamaterial interacts the most with incoming external sound pressures. Air at the Air jet m neck Neck of Air at Inside air bottle atmospheric compressed FigureFigure 1. Phenomenon 1. Phenomenon of Helmholtz of Helmholtz resonance resonance where where air in airside inside the cavity the cavity is modelled is modelled as a spring as a spring massmass system system (redrawn (redrawn from from[24]). [ 24]). Sui etSui al. et [25] al. designed [25] designed and tested and tested light-weight light-weight yet sound-proof yet sound-proof acoustic acoustic metamaetrials metamaetrials made made of of hexagonalhexagonal honeycomb honeycomb structure structure covered covered by by a arubbery rubbery memberane memberane sheet. CoveringCovering thethe sandwich sandwich panel panelwith with the the membrane membrane resulted resulted in an in increasedan increased sound sound transmission transmission loss up loss to 25updB to at25f dB= 200 at f Hz= 200. In Hz. another In anotherhoneycomb-based honeycomb-based structure, structure, Claeys etClaeys al. [26 ]et introduced al. [26] introduced a vibro-acoustic
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