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水声材料性能的自由场宽带压缩脉冲叠加法测量 总被引:9,自引:1,他引:9
水声材料的许多声学特性一般可以通过对复反射系数和透射系数计算得到。本文提出一种新的自由场测量方法,即应用宽带脉冲压缩技术在消声水池中测量有限尺寸的大面积材料样品的性能参数,从而使这种标准测量的低频限被明显降低。除传统的回声降低和插入损失参数等外,两个新的参数——消声系数和去耦系数也在评价之列。文中对两块平板样品进行了实验测量,其尺寸约为1m×1m,测量频率范围为 2~20kHz。 相似文献
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一种新的水声无源材料声学性能测量装置 总被引:1,自引:0,他引:1
阐述了一种新的水声无源材料声学性能实验室测量装置,测量频率范围10-100kHz,最大静水压至3.0MPa,被测材料样品典型尺寸为300×300mm2。装置应用多基元平面换能器基阵,大面积声透明PVDF薄膜水听器以及宽带窄脉冲信号和现代信号处理技术,在小型压力罐中建立近似的平面波自由声场,测量材料声学性能随频率、静水压的变化规律。测量参数包括复反射系数(口声降低)、复透射系数(插入损失)、衰减系数、复声阻抗和纵波声速。通过对多种不同性能材料样品的测量分析,验证了本装置的测量能力,装置的稳定性考核表明其反射测量扩展不确定度为1.2dB,透射测量扩展不确定度为0.8dB。 相似文献
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设计了一种原波频率500 kHz、差频范围1~30 kHz的截断宽带参量阵,作为水声材料测量系统的声源。通过分析典型频率下的宽带参量源指向性理论计算和实际测量结果,发现两者结果的曲线基本吻合,证明计算模型是正确的。应用钟形短时脉冲实现水声材料声特性的宽带测量,有益于降低样品边缘衍射干扰。并建立了测量水声材料大面积板状样品声压反射系数、声压透射系数和吸声系数的压力罐测量系统,罐体内尺寸Φ4 m×12 m,最高静水压4.5 MPa,测量频率范围1~30 kHz。对标准样品(尺寸1m×1m)进行了测量实验,其测量结果和理论曲线有很好的吻合,参量源测量法得到了验证;之后,通过对一块橡胶板样品在不同静压力下的吸声性能进行了测量和有效评估,进一步确认了参量源测量法在压力罐这样有限水域中的潜在应用价值。 相似文献
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水声材料低频声性能的行波管测量 总被引:3,自引:0,他引:3
发展了一种测量水声材料声学性能的行波管测量技术,能够在实验室充水管中模拟海洋水温水压环境,对样品的声学参数实施低频范围的测量。被测样品置于声管中央,声管两端配置一对发射器。应用主动消声技术使样品的透射声波在声管次发射器表面的反射可忽略,在管中建立起行波声场。然后,通过分别计算样品两边声场中每一对水听器的传递函数,得到样品的反射系数和透射系数。测量系统声管的内径为Φ208 mm,工作频率范围为100~4000 Hz,最高静水压为5 MPa。对水层和层状不锈钢样品的反射系数和透射系数进行了实际测量和理论计算,结果表明,测量值和计算值有较好的吻合,测量不确定度不大于1.5 dB。 相似文献
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A truncated broadband parametric array with a primary frequency of 500 kHz and difference frequency range of 1 kHz to 30 kHz was designed as a sound source of the underwater acoustic material measurement system.By analyzing the theoretical calculation and actual measurement results in array directivity of the truncated broadband parametric source at typical frequencies,we observed that the curves of the two results were basically consistent,which proved that the calculation model was correct.App... 相似文献
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A method suppressing multipath effect when measuring the underwater acoustic materials in a reverberant field is proposed, which is called "virtual end-fire array method".To weaken the coherence of the same-frequency reflection interference of each path, signal of different phases at different positions was transmitted by a single transducer in the simulation design, and a sharp directionality in the direction of the array length was formed. All signals at the above positions were superimposed t... 相似文献
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V. I. Klyachkin 《Acoustical Physics》2004,50(4):438-445
Statistical characteristics of an acoustic field that are based on the data of simultaneous measurements of pressure and acoustic velocity vector are investigated. Conditions of the formation of vector-phase characteristics of acoustic field are formulated in relation to the dispersion properties of the medium. Crosscorrelation functions of the components of the vector field are presented. Expressions for the characteristic functionals of vector-phase relationships in acoustic fields and, in particular, for the acoustic energy flux are derived with the use of functional methods. Algorithms of space-time processing of the energy flux vector and the optimum measurement algorithm for a Gaussian vector-phase field are considered. The signal-to-noise ratio is determined as the quality index of vector reception algorithms, and its relation to the corresponding parameter of scalar pressure field measurements is revealed. Indices of relative efficiency of vector algorithms are determined depending on the dispersion characteristics of the medium (the flux algorithm) and the dimension of the input vector of observations (the optimum algorithm). 相似文献