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Evaluation of Electro-Acoustic Techniques for In-Situ Measurement of Acoustic Absorption Coefficient of Grass and Artificial Turf Surfaces

机译:用于原位测量草和人造草皮表面的原位测量的电声技术评价

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The classical methods of measuring acoustic absorption coefficient using an impedance tube and a reverberation chamber are well established. However, these methods are not suitable for in-situ applications. The two in-situ methods; single channel microphone (P-probe) and dual channel acoustic pressure and particle velocity (Pu-probe) methods based on measurement of impulse response functions of the material surface under test, provide considerable advantage in data acquisition, signal processing, ease and mobility of measurement setup. This paper evaluates the measurement techniques of these two in-situ methods and provides results of acoustic absorption coefficient of a commercial artificial Astroturf, a Dow quash material, and a grass surface. The single channel microphone method uses impulse response calculations from a Maximum Length Sequence (MLS) signal excitation of an electro-acoustic loudspeaker and a Fast Hadamard Transformation (FHT) based cross-correlation algorithm by the deconvolution of recorded single-channel microphone signal and the input MLS signal. The dual-channel Pu-probe method is based on calculation of the complex impedance of the material surface under test from the frequency response function between the sound pressure and particle velocity time domain signals measured simultaneously at the same position on a material. The complex reflection coefficient calculated from both these methods further provides the acoustic absorption coefficient of the material under test.
机译:使用阻抗管和混响室测量吸声系数的经典方法已经很好地建立。然而,这些方法并不适合现场应用。两个原位方法;单声道麦克风(P-探针)和双通道声压和粒子速度(PU-探针)的基础上的下测试材料表面的脉冲响应函数的测量方法,在数据采集,信号处理,易用性和机动性提供相当大的优势测量设置。本文评估的这两种原位方法的测量技术,并且提供商用人工人工草皮,陶氏撤销材料和草表面的吸声系数的结果。单声道麦克风方法使用从最大长度序列由记录单声道麦克风信号和所述的解卷积的基于互相关算法的脉冲响应的计算(MLS)的电声扬声器和快速Hadamard变换(FHT)的信号激励输入MLS信号。双通道浦探针法是基于从下在对材料的同一位置同时测量的声压和粒子速度的时域信号之间的频率响应函数测试材料表面的复阻抗的计算。从这两种方法所计算的复反射系数进一步提供被测材料的吸声系数。

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