Bias Flow Acoustic Liner with Straight and Tapered Apertures

Soufiane Ramdani, N. Yamasaki, Y. Inokuchi, T. Ishii
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When a bias flow is introduced, the absorption coefficient reaches its maximum absorption of the incident sound wave in the region near the resonant frequency for a Mach number close to 9.71 . 2D numerical simulations are performed and validated with the experimental results. Good agreement is obtained for the majority of the simulated cases. Vortex shedding and its effect on the absorption coefficients is also investigated. INTRODUCTION Acoustic liners are widely used devices in aero-engines, and they are installed on the inner side of the nacelle to reduce fan noise in turbofan engines of commercial airplanes (conventional acoustic liners without bias flow). They are also used in the combustion chamber to reduce the acoustic instabilities caused by the combustion (acoustic liners with bias flow where the bias flow is caused by secondary air flow). An acoustic liner is typically made of a perforated metal sheet backed by a cavity. Each aperture of the perforated sheet and the cavity form a Helmholtz resonator. The resonator effectively absorbs the sound near the resonant frequency, however, its absorbing performance decreases at off-resonant frequencies. Howe [1] theoretically proposed that a low frequency (low Strouhal number) sound wave can be significantly attenuated by a jet flow by converting the acoustical energy into energy of fluctuating vorticity, which is shed from the nozzle edge. Bechert [2] proposed another theory to explain this phenomenon, and this was supported via experimental data. Bechert [2] also proposed a simple theory to predict the optimum Mach number of bias flow to obtain the perfect attenuation. On the other hand, Howe's theory to predict the sound absorption coefficient including the effects of a bias flow is well supported by an experiment by Hughes and Dowling [3]. Hence, this led to the idea that the off-resonant performance of a resonator can be improved if a jet (or a bias flow) is introduced from an aperture of an acoustic liner. Lahiri et al. [4] collected this type of experimental data and showed that the application of a bias flow through the aperture widens the frequency range of dissipation, with the penalty of reduced peak performance near the resonant frequency. Zhao and Li [5] wrote a summary on tunable acoustic liners including a liner with bias flow. In the field of numerical simulation, Mendez and Eldredge [6] performed a 3D large eddy simulation (LES), and Ji and Zhao [7] performed a 2D lattice Boltzman method (LBM) for an aperture with bias flow, and both made a comparison with Howe's theory, obtaining good agreements. Roche et al. [8] conducted 3D and 2D axisymmetric numerical simulations for a cylindrical acoustic resonator in the case without a bias flow using direct numerical simulation (DNS). Good agreement was obtained between 2D and 3D results. In a previous study (Ramdani et al. [9]), 2D simulations of a slit resonator were conducted using LES for cases with and without bias flow. Good agreement was obtained for the non-bias flow case. However, the bias flow case was not validated due to the lack of the experimental results for the simulated model. Tam et al. [10] conducted a series of experiments and DNS simulations to slit apertures with a 90° corner (straight aperture) and 45° corner (tapered aperture). The results obtained using the simulation supports the usage of computational aeroacoustics (CAA) as a design tool. Wada and Ishii [11] performed experiments for acoustic liners with a bias flow passing through the apertures of a perforated plate (circular straight perforations) and observed that the absorption range of the liner became wider and was not concentrated around the resonant frequency as in the case of the conventional liner. They compared the experimental results with Howe's extended theory proposed by Luong et al. [12], which considered the thickness of the perforated sheet and obtained good agreements. In a previous study (Tanaka et al. [13]), the macroscopic effect of the design parameters (such as the shape of the aperture and the flow velocity when a bias flow is applied through the aperture) on the impedance of an acoustic resonator was experimentally investigated via an acoustic impedance tube. The results revealed that the fully tapered aperture exhibited a wider absorption frequency range when compared to that of a straight circular aperture. However, little was known about the reason for such a behavior given the difficulty of visualizing the flow around the small apertures in the experimental setup using the impedance tube. In the present study, the acoustic performance of the liner and the flow field around the perforated plate is numerically solved using the compressible Navier Stokes equations to understand the acoustic and fluid dynamic behavior of the liner and the effect of the shape of the perforation at a microscopic level. Bias Flow Acoustic Liner with Straight and Tapered Apertures Soufiane Ramdani1, Nobuhiko Yamasaki1, Yuzo Inokuchi2, Tatsuya Ishii3 1 Department of Aeronautics and Astronautics Kyushu University 744 Motooka, Nishi-ku, Fukuoka 819-0395, JAPAN 2Civil Aviation College 3Japan Aerospace Exploration Agency International Journal of Gas Turbine, Propulsion and Power Systems June 2019, Volume 10, Number 3 Manuscript Received on October 17, 2018 Review Completed on June 27, 2019 Copyright © 2019 Gas Turbine Society of Japan","PeriodicalId":38948,"journal":{"name":"International Journal of Gas Turbine, Propulsion and Power Systems","volume":"1 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2019-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Gas Turbine, Propulsion and Power Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.38036/jgpp.10.3_1","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"Engineering","Score":null,"Total":0}
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Abstract

Experimental and computational studies are performed on slit resonators, i.e., one aperture with a high aspect ratio that spans through the center of the plate. An impedance tube experiment is conducted to investigate the macroscopic response of slit apertures. The test specimens include straight and tapered apertures. Subsequently, the effect of introducing a bias flow is investigated. The absorption performance increases when the sound pressure level increases to a level that causes a production of shed vortices. When a bias flow is introduced, the absorption coefficient reaches its maximum absorption of the incident sound wave in the region near the resonant frequency for a Mach number close to 9.71 . 2D numerical simulations are performed and validated with the experimental results. Good agreement is obtained for the majority of the simulated cases. Vortex shedding and its effect on the absorption coefficients is also investigated. INTRODUCTION Acoustic liners are widely used devices in aero-engines, and they are installed on the inner side of the nacelle to reduce fan noise in turbofan engines of commercial airplanes (conventional acoustic liners without bias flow). They are also used in the combustion chamber to reduce the acoustic instabilities caused by the combustion (acoustic liners with bias flow where the bias flow is caused by secondary air flow). An acoustic liner is typically made of a perforated metal sheet backed by a cavity. Each aperture of the perforated sheet and the cavity form a Helmholtz resonator. The resonator effectively absorbs the sound near the resonant frequency, however, its absorbing performance decreases at off-resonant frequencies. Howe [1] theoretically proposed that a low frequency (low Strouhal number) sound wave can be significantly attenuated by a jet flow by converting the acoustical energy into energy of fluctuating vorticity, which is shed from the nozzle edge. Bechert [2] proposed another theory to explain this phenomenon, and this was supported via experimental data. Bechert [2] also proposed a simple theory to predict the optimum Mach number of bias flow to obtain the perfect attenuation. On the other hand, Howe's theory to predict the sound absorption coefficient including the effects of a bias flow is well supported by an experiment by Hughes and Dowling [3]. Hence, this led to the idea that the off-resonant performance of a resonator can be improved if a jet (or a bias flow) is introduced from an aperture of an acoustic liner. Lahiri et al. [4] collected this type of experimental data and showed that the application of a bias flow through the aperture widens the frequency range of dissipation, with the penalty of reduced peak performance near the resonant frequency. Zhao and Li [5] wrote a summary on tunable acoustic liners including a liner with bias flow. In the field of numerical simulation, Mendez and Eldredge [6] performed a 3D large eddy simulation (LES), and Ji and Zhao [7] performed a 2D lattice Boltzman method (LBM) for an aperture with bias flow, and both made a comparison with Howe's theory, obtaining good agreements. Roche et al. [8] conducted 3D and 2D axisymmetric numerical simulations for a cylindrical acoustic resonator in the case without a bias flow using direct numerical simulation (DNS). Good agreement was obtained between 2D and 3D results. In a previous study (Ramdani et al. [9]), 2D simulations of a slit resonator were conducted using LES for cases with and without bias flow. Good agreement was obtained for the non-bias flow case. However, the bias flow case was not validated due to the lack of the experimental results for the simulated model. Tam et al. [10] conducted a series of experiments and DNS simulations to slit apertures with a 90° corner (straight aperture) and 45° corner (tapered aperture). The results obtained using the simulation supports the usage of computational aeroacoustics (CAA) as a design tool. Wada and Ishii [11] performed experiments for acoustic liners with a bias flow passing through the apertures of a perforated plate (circular straight perforations) and observed that the absorption range of the liner became wider and was not concentrated around the resonant frequency as in the case of the conventional liner. They compared the experimental results with Howe's extended theory proposed by Luong et al. [12], which considered the thickness of the perforated sheet and obtained good agreements. In a previous study (Tanaka et al. [13]), the macroscopic effect of the design parameters (such as the shape of the aperture and the flow velocity when a bias flow is applied through the aperture) on the impedance of an acoustic resonator was experimentally investigated via an acoustic impedance tube. The results revealed that the fully tapered aperture exhibited a wider absorption frequency range when compared to that of a straight circular aperture. However, little was known about the reason for such a behavior given the difficulty of visualizing the flow around the small apertures in the experimental setup using the impedance tube. In the present study, the acoustic performance of the liner and the flow field around the perforated plate is numerically solved using the compressible Navier Stokes equations to understand the acoustic and fluid dynamic behavior of the liner and the effect of the shape of the perforation at a microscopic level. Bias Flow Acoustic Liner with Straight and Tapered Apertures Soufiane Ramdani1, Nobuhiko Yamasaki1, Yuzo Inokuchi2, Tatsuya Ishii3 1 Department of Aeronautics and Astronautics Kyushu University 744 Motooka, Nishi-ku, Fukuoka 819-0395, JAPAN 2Civil Aviation College 3Japan Aerospace Exploration Agency International Journal of Gas Turbine, Propulsion and Power Systems June 2019, Volume 10, Number 3 Manuscript Received on October 17, 2018 Review Completed on June 27, 2019 Copyright © 2019 Gas Turbine Society of Japan
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带有直孔和锥形孔的偏流声学衬垫
在狭缝谐振器上进行了实验和计算研究,即一个具有高宽高比的孔径穿过板的中心。采用阻抗管实验研究了狭缝孔径的宏观响应。试件包括直孔和锥形孔。随后,研究了引入偏置流的影响。当声压级增加到产生脱落涡的水平时,吸收性能提高。当引入偏置流时,在马赫数接近9.71时,入射声波的吸收系数在谐振频率附近区域达到最大值。进行了二维数值模拟,并与实验结果进行了验证。大多数的模拟案例都得到了很好的吻合。研究了旋涡脱落及其对吸收系数的影响。声学衬垫是航空发动机中广泛使用的装置,它安装在商用飞机涡扇发动机的机舱内侧,以降低风扇噪声(传统的无偏流声学衬垫)。它们也用于燃烧室,以减少由燃烧引起的声学不稳定性(带有偏置流的声学衬垫,其中偏置流是由二次空气流动引起的)。声学衬垫通常由穿孔金属板制成,后面有一个腔。穿孔片的每个孔和腔形成一个亥姆霍兹谐振腔。谐振器在谐振频率附近的吸声效果较好,在非谐振频率处吸声效果较差。Howe[1]从理论上提出,射流通过将声能转化为波动涡量的能量,从喷管边缘流出,可以显著地衰减低频(低斯特罗哈尔数)声波。Bechert[2]提出了另一种理论来解释这一现象,并得到了实验数据的支持。Bechert[2]也提出了一个简单的理论来预测偏置流的最佳马赫数,以获得完美的衰减。另一方面,Hughes和Dowling的实验也很好地支持了Howe预测包括偏置流影响的吸声系数的理论。因此,这导致了这样的想法,即如果从声学衬垫的孔径引入射流(或偏置流),则可以改善谐振器的非谐振性能。Lahiri et al.[4]收集了这类实验数据,并表明通过孔径施加偏置流会使耗散的频率范围变宽,其代价是在谐振频率附近峰值性能降低。Zhao和Li[5]写了一篇关于可调声学衬垫的综述,其中包括一个带有偏流的衬垫。在数值模拟领域,Mendez和Eldredge[6]对偏流孔径进行了三维大涡模拟(LES), Ji和Zhao[7]对偏流孔径进行了二维晶格玻尔兹曼方法(LBM),并与Howe理论进行了比较,得到了很好的一致性。Roche等人使用直接数值模拟(DNS)对无偏置流情况下的圆柱形声学谐振器进行了三维和二维轴对称数值模拟。二维和三维结果吻合较好。在之前的一项研究中(Ramdani et al.[9]),使用LES对狭缝谐振器进行了有偏流和无偏流情况下的二维模拟。在无偏流情况下,得到了很好的一致性。然而,由于缺乏模拟模型的实验结果,因此没有对偏流情况进行验证。Tam等人([10])进行了一系列实验和DNS模拟,以90°角(直孔径)和45°角(锥形孔径)的方式切开孔径。仿真结果支持了计算气动声学(CAA)作为设计工具的使用。Wada和Ishii[11]对有偏流通过穿孔板(圆形直孔)的声学衬垫进行了实验,观察到衬垫的吸收范围变得更宽,并且不像传统衬垫那样集中在共振频率周围。他们将实验结果与Luong et al.[12]提出的Howe扩展理论进行了比较,该理论考虑了穿孔板的厚度,得到了很好的一致性。在之前的一项研究中(Tanaka et al.[13]),通过声阻抗管实验研究了设计参数(如孔径形状和偏置流通过孔径时的流速)对声谐振器阻抗的宏观影响。结果表明,与直圆孔径相比,全锥形孔径具有更宽的吸收频率范围。 然而,考虑到在实验装置中使用阻抗管可视化小孔径周围的流动的困难,人们对这种行为的原因知之甚少。本文采用可压缩Navier - Stokes方程对内衬的声学性能和穿孔板周围的流场进行了数值求解,以在微观水平上了解内衬的声学和流体动力学行为以及穿孔形状的影响。直孔和锥孔偏流声学内衬Soufiane Ramdani1, Nobuhiko Yamasaki1, Yuzo Inokuchi2, Tatsuya ishii31 1九州大学航空航天系744 Motooka, nishiku, Fukuoka 819-0395, JAPAN 2民航学院3日本宇宙航空研究开发机构国际燃气轮机,推进和动力系统学报2019年6月,第10卷,第3期手稿接收于2018年10月17日,评审于6月27日完成2019版权所有©2019日本燃气轮机协会
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