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1.
高声压级时多孔金属板的吸声特性研究   总被引:6,自引:0,他引:6  
彭锋  王晓林  孙艳  常宝军  刘克 《声学学报》2009,34(3):266-274
针对高声压级下有限厚度多孔金属板在线性阻抗背衬条件下(背衬表面声压与声质点速度为线性关系)的吸声问题,提出了一个描述不同声压级下材料层法向吸声性能的一维模型,并给出求解材料层内部声质点速度的线化与差分方法,以预测多孔金属板在高声压级下的非线性吸声特性。在阻抗管中对两块多孔金属板进行了声学测试,得到了材料层法向表面阻抗和吸声系数随入射声压级变化的实验结果。研究表明:实验与理论预测符合良好,验证了模型与数值方法的正确性。本文所提原理和方法,可用于一般硬质多孔材料。   相似文献   

2.
陈昕  赵静  陈志菲  侯宏  鲍明  杨建华 《应用声学》2023,42(6):1207-1214
使用不同声源利用矢量传声器对毛毡材料进行现场吸声系数测试,研究了不同背景下不同声源的抗噪能力。矢量传声器可以同时测得声压和质点振速信号,进而可计算得到阻抗,利用自由空间和材料表面的阻抗可计算得到材料的吸声系数。在此次试验中,使用不同声源分别在无干扰和有一白噪声干扰源的两种情况下进行测试。结果表明,使用对数扫频脉冲和巴特沃斯脉冲测试所得的吸声系数曲线更平滑,说明脉冲声可以有效降低环境反射的影响,在高噪声背景下使用对数扫频脉冲测试所得的结果基本没有受到背景噪声的影响,说明对数扫频脉冲的抗噪能力更强。因此,使用对数扫频脉冲作为声源进行测试可有效减弱环境反射和背景噪声的影响。  相似文献   

3.
提出了一种利用矢量水听器在声管中实现一体化有源吸声终端的方法。该吸声终端采用矢量水听器作为传感元件,以实现入射波和反射波的分离,克服了传统双水听器声波分离方法中传感器间距及测量频率的限制,显著拓宽了一体化有源吸声终端的低频吸声频段。由声管中水声材料的测试原理出发,重点分析了吸声终端中传感元件灵敏度误差对吸声终端性能的影响,并给出了反射、透射系数的修正方法。实验结果表明:该有源吸声终端在100~2000 Hz频段内吸声系数可以达到0.98以上,测量得到材料的声压反射系数、声压透射系数及理论计算基本一致。   相似文献   

4.
孙中政  韩旭  王宇飞 《声学学报》2022,47(2):229-240
为了测量高频材料吸声系数,采用声模态分解的方法,基于阻抗管构建测试设备,在阻抗管内测量超过平面波截止频率的的高频吸声系数.测量过程中,通过在阻抗管的周向和轴向分别布置传声器阵列,分离管道内前3阶周向声模态以及各阶声模态的轴向传播入射波和反射波,从而得到最高频率达10000 Hz的材料吸声系数,并通过对比常规阻抗管测试方...  相似文献   

5.
针对现有方法对材料吸声系数进行现场测量时存在低频测量误差大的问题,本文提出了一种利用扬声器线阵列对材料吸声系数进行现场测量的新方法。该方法使用基于能量比值约束的最小二乘法在待测材料表面进行平面波声场重建并结合双传声器传递函数法对材料的吸声系数进行测量。数值仿真表明在100~1600 Hz频率范围内,新方法在未加约束时能够对材料的吸声系数进行准确测量。在半消声室中利用新方法测量了三聚氰胺泡沫的吸声系数,分析了能量比值约束值对测量结果的影响,并和阻抗管以及其它两种现场测量方法的测量结果进行了对比。结果表明该方法能够对吸声材料在160~1600 Hz频段内的吸声系数进行准确测量,并且相较于现存的现场测量方法,新方法具有更低的测量频率下限。  相似文献   

6.
陈继康 《应用声学》1988,7(1):19-22
本文报道了利用压强梯度法原理构成的便携式声强测量装置,该装置既能测量声强,也能测量声压的真有效值,还可以测量质点振动速度的真有效值,它是一种可以对声场的能量密度和能流密度进行综合分析的新型装置,为噪声分析,声功率测量和声源鉴别等项工作提供了一种新型测试手段。该装置能在100主5000Hz的频率范围内进行可靠的测量,使用方法简单,操作方便。  相似文献   

7.
材料吸声系数双传声器测量的参数识别方法   总被引:1,自引:0,他引:1       下载免费PDF全文
胡恒  郑四发  郝鹏  连小珉 《应用声学》2008,27(4):305-310
本文提出了在普通房间中利用双传声器对多孔性和纤维性吸声材料吸声系数测量时的参数识别方法。利用Delany&Bazley经验模型对测量数据进行了参数识别,建立了材料的阻抗模型,并计算出材料全频带的吸声系数。与驻波管方法得到的吸声系数相比,在0~3000Hz范围内,二者都能较好地吻合。通过在不同的环境中进行对比测试,说明该方法具有较好的重复性和准确性。  相似文献   

8.
基于矢量水听器的水下目标低频辐射噪声测量方法研究   总被引:17,自引:2,他引:15  
矢量水听器由声压传感器和质点振速传感器复合而成,可以空间共点、同步测量声压和质点振速的各正交分量。本文利用矢量水听器测量水下目标低频辐射噪声,给出了测量的基本原理。证明了:(1)在各向同性噪声场中质点振速的最大空间增益为约 4.8 dB;有功声强的空间增益与时间带宽积有关,(2)在各向异性场中,有功声强的空间增益取决于噪声场的空间分布。计算机仿真结果和海上试验结果也在文中给出。  相似文献   

9.
管束穿孔板的管腔耦合共振吸声机理研究   总被引:1,自引:0,他引:1       下载免费PDF全文
苏玉  梅中建  吕亚东  程晓斌 《声学学报》2021,46(6):1202-1211
为了揭示管束穿孔板共振吸声结构的吸声机理,利用热黏性条件下基于有限元算法的管束穿孔板仿真模型,研究了平面声波正入射条件下,管束穿孔板内部声场分布特征,并利用阻抗管对吸声系数的理论仿真结果进行了试验验证.结果表明,管束穿孔板在低频主要靠腔体共振吸声,在高频主要靠管共振吸声,管束穿孔板整体呈现出较为明显的管腔耦合共振吸声特征。管束穿孔板共振时管中声强和质点法向振速较大,高频次吸声峰频点处管中和腔中均有驻波形成,频率越高驻波数量越多.管束穿孔板的耦合共振受到管长、腔深、穿孔率和管内径等参数变化的影响,管长对高频耦合共振的影响最大,管长增大使高频主吸声峰频点移向低频,并使相邻主吸声峰之间的间距减小.   相似文献   

10.
楼华鼎  闵鹤群 《声学学报》2023,(5):1012-1020
针对尺寸显著小于阻抗管横截面的非标准尺寸样品,提出了一种阻抗管内非标准尺寸样品的正入射吸声系数测量方法,分析了其参数对测量结果的影响,并与标准尺寸样品(与阻抗管横截面相同)比较。首先在其旁布置一种具有特定声阻抗的同厚度的声学材料(PAM),形成与阻抗管横截面相同的表面平整的非连续阻抗试件(IAIS),然后根据GB/T 18696.2—2002测得IAIS表面声阻抗,并基于声电类比法计算得到非标准尺寸样品的表面声阻抗及其正入射吸声系数。结果表明,非标准尺寸样品的面积率越大或声扩散边界长度越小,该方法精度越高;当非标准尺寸样品为多孔材料时,选择非刚性的、声阻抗与之接近的PAM也可提高测量精度;而非标准尺寸样品为共振吸声结构时,选择刚性PAM时,本文方法仍具有一定精度。  相似文献   

11.
For modeling of jute as acoustic material, knowledge of its non-acoustical parameters like porosity, tortuosity, air flow resistivity, thermal and viscous characteristic lengths is a prime requisite. Measurement of these non-acoustical parameters is not straightforward and involves a dedicated measurement setup. So in order to overcome this issue, the inverse acoustical characterization can be used. In this paper, the particle swarm optimization method (PSO) is used as an optimization method. This method estimates the non-acoustical parameters of jute material in felt form by minimizing the error between experimental and theoretical sound absorption data. In this work, the impedance prediction models for fibrous materials like Johnson–Champoux–Allard model with rigid and limp frame and Garai–Pompoli model is used for sound absorption coefficient calculation by the transfer matrix method along with the PSO. The inverse estimated non-acoustical parameters for jute material are then compared with estimated and experimentally measured parameters for jute felts. Using these inversely predicted parameters, sound absorption of multilayer sound absorbers is also studied.  相似文献   

12.
Helmholtz resonators with sound absorption materials filling the neck may have an improved sound absorption capacity. In this work, parallel perforated ceramics with different perforation diameters were installed into the neck of a Helmholtz resonator to improve its acoustic impedance to simultaneously achieve a better acoustic absorption coefficient and a wider absorption bandwidth. An experimental system was built to investigate the effect of the perforation diameters on the sound absorption performance of the resonator. It is found that nonlinear effects near the resonance frequency affect the resonator?s neck mouth impedance and further its sound absorption performance significantly. For frequency range 50–500 Hz, a model of the neck mouth impedance is developed based on a revised Forchheimer relationship. The experimental results are in good agreement with the theoretical model.  相似文献   

13.
The absorption coefficient of acoustic materials can be measured either in the frequency or the time domain. At normal incidence, a sample of the material is fitted within an impedance tube and the absorption coefficient is calculated in the frequency domain from the measurement of the transfer function between two microphones [ISO 10534-2. Acoustics - determination of sound absorption coefficient and impedance in impedance tubes - Part 2: transfer function method. ISO, Geneva, Switzerland; 1996]. When the acoustic material must be characterized at oblique incidence or in situ (noise barriers, for instance) the absorption coefficient is calculated from measurements of the loudspeaker-microphone impulse response in the time domain, both in free field and in front of the sample [CEN/TS 1793-5. Road traffic noise reduction devices - test method for determining the acoustic performance - Part 5: intrinsic characteristics - in situ values of sound reflection and airborne sound insulation. CEN, Brussels, Belgium; 2003, ISO 13472-1. Acoustic measurement of sound absorption properties of road surfaces in situ - Part I: extended surface method. ISO, Geneva, Switzerland; 2002]. Since the absorption is an intrinsic property of the acoustic material, its measurement in either domain must provide the same result. However, this has not been formally demonstrated yet. The aim of this paper is to carry out a comparison between the absorption coefficient predicted by the impedance model of a Microperforated Insertion Unit and the absorption coefficient predicted from a simulated reflection trace taken into account the finite length of the time window.  相似文献   

14.
The pressure-particle velocity (PU) impedance measurement technique is an experimental method used to measure the surface impedance and the absorption coefficient of acoustic samples in situ or under free-field conditions. In this paper, the measurement uncertainty of the the absorption coefficient determined using the PU technique is explored applying the Monte Carlo method. It is shown that because of the uncertainty, it is particularly difficult to measure samples with low absorption and that difficulties associated with the localization of the acoustic centers of the sound source and the PU sensor affect the quality of the measurement roughly to the same extent as the errors in the transfer function between pressure and particle velocity do.  相似文献   

15.
A new empirical model has been developed by the authors to predict the flow resistivity, acoustic impedance and sound absorption coefficient of polyester fibre materials. The parameters of the model have been adjusted to best fit the values of airflow resistivity and sound absorption coefficient measured over a set of 38 samples. Calculated results are compared with normal incidence measurements carried out using two different techniques: the transfer-function method in an impedance tube (ISO 10534-2) and the free-field impulse response method (ISO 13472-1). Measurements performed on polyester fibre materials with different density and thickness values, and diameter ranging from 18 to 48 μm, are in good agreement with the predictions of the new model. It is concluded that the new model can predict the basic acoustic properties of common polyester fibre materials with any practical combination of thickness and density2.  相似文献   

16.
This paper presents a straightforward application of an indirect method based on a three-microphone impedance tube setup to determine the non-acoustic properties of a sound absorbing porous material. First, a three-microphone impedance tube technique is used to measure some acoustic properties of the material (i.e., sound absorption coefficient, sound transmission loss, effective density and effective bulk modulus) regarded here as an equivalent fluid. Second, an indirect characterization allows one to extract its non-acoustic properties (i.e., static airflow resistivity, tortuosity, viscous and thermal characteristic lengths) from the measured effective properties and the material open porosity. The procedure is applied to four different sound absorbing materials and results of the characterization are compared with existing direct and inverse methods. Predictions of the acoustic behavior using an equivalent fluid model and the found non-acoustic properties are in good agreement with impedance tube measurements.  相似文献   

17.
吸声型薄膜声学超材料低频宽带吸声性能研究*   总被引:1,自引:1,他引:0       下载免费PDF全文
本文根据吸声型薄膜声学超材料的吸声机理,在传统的吸声型薄膜声学超材料结构的基础上引入质量非对称结构, 优化了不同厚度质量片的排布方式,并根据优化结果制备了能够实现低频宽带吸声效果的薄膜声学超材料样品。对其进行声学实验的测试结果显示,样品在 100-1000Hz 频率范围内的平均吸声系数达 0.25,并在 250-800Hz 频率范围内出现了多个共振吸收峰,且实验测得的吸声系数曲线与仿真曲线的趋势有较高的一致性。因此该样品实现了低频宽带吸声。  相似文献   

18.
孙阳  华波 《应用声学》2018,37(4):540-550
利用阻抗管法测量吸声系数是水下吸声材料研制过程中的重要环节,实验测量结果相比理论计算结果更具说服力。然而在待测样品的制备和安装过程中容易引入的系统误差往往被忽略,从而影响实测结果可信度。为了降低系统误差,本文提出缝隙宽、垂直度和光洁度三种可能引入系统误差的因素,搭建传递函数法水下吸声系数测量的有限元模拟实验环境并验证仿真计算算法的正确性,研究相关参量对橡胶吸声系数的影响规律,并给出一定误差下对相关参量的限制要求。所得结论对降低测量误差、提升实测结果可信度具有一定参考价值。  相似文献   

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