超声波透射法检测水泥模块的缺陷

介绍了超声波透射法检测水泥模块中缺陷的基本原理,并通过对自制水泥试块的检测,研究了不同缺陷对声学参量的影响.测试结果表明:有缺陷模块会使检测超声波比正常传播时声时变大(声速变小),波幅明显衰减,波形产生畸变,频率也会发生异常波动.因此,评价水泥模块的缺陷时要将声时、幅值、频率、波形结合起来,综合分析异常变化来确定缺陷的性质.     

岩石中孔隙流体含量对超声波衰减影响的实验研究

目前,关于岩石中孔隙流体含量对超声波衰减影响的实验数据还很少。本文介绍的由瞬态波形存贮器和微机控制系统组成的超声波信号采集与数字处理系统,适于实验室内测量超声衰减与流体含量的变化关系。作者以砂岩试件作了实验并取得一些有价值的数据。 实验研究结果,表明砂岩中横波衰减随饱和度增加而增加,纵波衰减随饱和度增加有一个明显的峰值出现。砂岩中声波衰减的品质因数Q值比声波速度v值反映岩石的物理力学性质更灵敏。从所得数据看,同一岩石的Q值随含水量变化量为速度变化量的五倍以上。     

三点弯曲试验 条件下花岗岩声发射横纵波特征及损伤演化*

开展花岗岩三点弯曲试验,利用横纵波两种传感器接收花岗岩破坏过程的声发射信号,对比分析声发射横纵波信号的时频特征,在此基础上,基于声发射横纵波建立损伤变量,探讨花岗岩三点弯曲条件下损伤演化规律。研究结果表明：花岗岩破坏过程声发射横纵波事件率变化趋势较为相似,临近峰值载荷时均加速上升,破坏时达到峰值,但纵波事件率加速点早于横波事件率;声发射横纵波能率变化趋势一致,呈现峰前低水平稳定变化、峰后陡升到峰值的特征。声发射横纵波主频在临近峰值载荷逐渐形成主频条带,但其频率存在差异,纵波主频分布在0~10 kHz、30~50 kHz和100~110 kHz,而横波主频集中分布在0~10 kHz。相比纵波损伤变量,横波损伤变量能够刻画峰后损伤急速发展的过程,能较好地表征花岗岩三点弯曲作用下损伤变化规律。     

变压器寄生参数和负载特性对高压脉冲波形的影响

构建了输出电压幅值为0～20 kV、脉冲重复频率为0.25～20 kHz的双极性高压脉冲电源实验平台,研究了变压器寄生参数与负载特性对输出脉冲波形的影响。采用等效电路复频域解析方法,分析了变压器寄生参数对输出脉冲波形的上升沿、平顶及下降沿的影响规律,并通过改变变压器绕线方案间接验证。发现变压器分布电容和漏感越大,输出脉冲波形上升沿与下降沿越平缓,过冲电压幅值越大,并采用脉冲变压器二次侧均匀密绕、一次侧均匀疏绕、高匝数的方案进行优化。进一步分析了纯阻性、阻容性或阻感性负载特性对输出高压脉冲波形的影响规律,发现电阻值增大（5～50 kΩ）,过冲电压幅值增大,脉冲上升沿和下降沿变陡;当负载电阻回路串联小电容时,过冲电压幅值显著增大,而电容值高于一定值时输出脉冲波形恢复至与纯电阻波形一样;当负载电阻回路串联电感时,输出脉冲波形下降沿变平缓。     

一种新的水声无源材料声学性能测量装置

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300×300mm~2。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。     

4.0 GPa压力下纯橄岩弹性纵波速度和衰减的实验研究

 应用超声波透射法和超声波频谱振幅比法、在4.0 GPa压力条件下、测量了弹性纵波通过纯橄岩的波速（v_P）和品质因子值（Q_P，用于表征衰减）随压力的变化，并分析了纯橄岩内部结构的变化对波速和衰减的影响。在实验压力范围内（≤4.0 GPa），随压力升高，纯橄岩的纵波速度逐渐增大：从7.6 km/s（0.4 GPa）逐渐增大至8.5 km/s（4.0 GPa），升高了11.8%，低压时的增大幅度大于高压时的增大幅度。纯橄岩的品质因子值呈两段式线性变化：从低压区间到高压区间品质因子值的增大幅度明显变小（0.4~2.4 GPa压力范围内Q_P增大了358.5%，2.4~4.0 GPa压力范围内Q_P仅升高了7.6%）。纯橄岩的品质因子从54（0.4 GPa）升高至266.4（4.0 GPa），增大幅度达393.3%。在相对低压（0.4~2.4 GPa）条件下，纵波通过纯橄岩的速度增大、衰减降低主要是由于样品内的孔隙和微裂纹大量闭合，岩石密度增大，纵波在通过样品内孔隙和裂缝时损失的机械能降低，因此纵波通过纯橄岩的能量增大（即衰减降低），波速升高；当围压较高（2.4~4.0 GPa）时，纯橄岩内大部分裂纹已经闭合，而且矿物颗粒边界接触紧密。岩石内部的裂纹和颗粒之间由于摩擦滑动而损失的能量也变少，所以在高压时纯橄岩的波速和衰减的变化幅度变缓，但波速仍呈线性增大，而品质因子值（衰减）随压力升高几乎趋于不变。     

黏弹材料动力学参数的宽频测试

利用改进的波速法,对黏弹性材料连续宽频范围的动力学参数进行测试。利用有限元方法,对波速法的测试过程进行了仿真,验证了利用长短棒波速法测量宽频动力学参数的有效性。采用可控脉冲生成技术,在激振器上产生了用于宽频测试的短脉冲信号。黏弹性长短棒在上述宽带短脉冲激励下作纵向强迫振动,利用激光测振仪测量长短两棒自由端的纵向振动速度,从而可得两振动信号在连续宽频范围的幅值比和相位差,进而可根据波速法原理计算得到材料在连续宽频范围的储能模量和损耗因子。测试结果表明,该系统通过较少次数测试,可直接计算得到1~5 kHz连续宽频范围的动力学参数,测试结果与黏弹仪数据吻合。通过对幅值比和相位差进行线性最小二乘拟合,可以进一步拓展测量的频率范围。该方法准确可靠、简便快速,具有实际应用价值。     

超声波和超声场

 声波是一种机械波,如果用频率来表征声波,并以人的感觉频率为分界线,可把声波划分为次声波(f<20Hz)可闻声波(20Hz≤f≤20kHz)及所谓超声波,它是指频率大于20kHz以上的声波。一般认为人耳所能听见频率的上限为20kHz。由于超声波的波长短,相同的振幅情况下,质点振动传递的能量就大得多,超声波在传播时就具有了与光传播时类似的特性,可以借助于光学的一些原理来研究它。计算表明,在液体中传播着超声波,其质点振动加速度的幅值可高达重力加速度的上百万倍!波长短的超声波的显著特征是方向性强,这样可用它采集信息,特别是材料内部的信息,因为超声波几乎能穿透任何材料。这对于某些其他辐射能量不能穿透的材料,超声波便显示出其独特的优越性。因之,超声波在工业、医疗等科技领域中有着重要的应用。     

纳秒激光诱导空气等离子体射频辐射特性研究

开展了波长为532 nm、脉宽为8 ns的纳秒激光诱导空气等离子体射频电磁辐射特性实验研究,基于锥形天线探测空气等离子体在30-800 MHz频谱范围有较强的射频电磁辐射,是等离子体内电偶极子振荡变速运动造成的.实验结果表明:随激光能量增加,30-200 MHz范围内射频辐射强度逐渐变强,但360-600 MHz频率范围射频辐射强度逐渐变弱.等离子体射频辐射的空间分布依赖于入射激光的偏振方向,当激光偏振方向与天线放置方向一致时,该方向上空气等离子体的射频辐射强度高,谱线较丰富.射频辐射总功率随激光能量先增加后降低,采用等离子体电子密度变化对等离子体频率及等离子体衰减系数影响(制约)关系,对射频辐射总功率随激光能量的变化规律进行了解释.     

二维圆盘颗粒体系声学行为的数值研究

数值测量了卸载过程中二维单分散圆盘颗粒系统的横波、纵波声速、声衰减系数、非线性系数随压强的变化以及声衰减系数随频率的变化.结果表明,二维(2D)圆盘颗粒体系的横波、纵波声速均随压强呈分段幂律标度:当压强P10~(-4)时,横波、纵波声速随压强的增大而减小;当P10~(-4)时,有v_t~P~(0.202),v_l~P~(0.338).进一步得到其剪切模量和体积模量的比值G/B也随压强呈幂律标度,G/B~P~(-0.502),暗示在低压强下,与三维(3D)球形颗粒体系类似,2D圆盘颗粒体系也处于L玻璃态.水平激励和垂直激励下2D圆盘颗粒系统的衰减系数随频率变化也呈现分段行为:当频率f0.05时,衰减系数不随f变化;当f0.05时,横波纵波的衰减系数α~f;当f0.35时,横波衰减系数α_T~f~2,纵波衰减系数α_L~f~(1.5).此外,竖直水平激励下的2D圆盘颗粒系统的非线性系数和衰减系数随压强也呈现与声速类似的分段规律:当P10~(-4)时,横波非线性系数β_T~P~(-0.230),其余都不随压强变化.当P10~(-4)时,两者均随压强增大呈幂律减小:β_T~P~(-0.703),β_L~P~(-0.684),α_T~P~(-0.099),α_L~P~(-0.105).进而得到2D圆盘颗粒系统中散射相关的特征长度?~*随压强呈幂律标度,当P10~(-4)时,?~*~P~(-0.595);当P10~(-4)时,?~*~P~(0.236).     

Experimental study of wave dispersion and attenuation in concrete

Results from an experimental study concerning wave propagation in cementitious materials are presented in this paper. Narrow band pulses at several frequencies were introduced into specimens of cement paste, mortar and concrete allowing direct measurement of longitudinal wave velocities and amplitude for each frequency. It is shown that aggregate content play an important role in wave propagation increasing considerably the wave velocity, while the aggregate size seems to control the attenuation observed. Slight velocity variations observed with frequency are discussed in relation to the degree of inhomogeneity of the materials.     

曲线坐标系下孔隙介质圆柱纵向表面波的传播特性

为了研究孔隙介质圆柱纵向表面波的传播规律,分析其频散和衰减特性,在正交曲线坐标系下建立了表面波的频散方程,通过数值计算得到频散曲线,将纵向导波最低模态与表面波进行对比,并分析了曲率半径及孔隙参数对表面波频散和衰减的影响。结果表明,当频率足够大时,导波最低模态的频散曲线与表面波近似;在同一频率下,表面波的相速度随曲率半径的增大而增大,随孔隙度的增大而减小;表面波的衰减随孔隙度的增大而增大。研究结果为开展孔隙介质圆柱结构的超声无损评价提供了一定的理论参考。     

无限流体中孔隙介质圆柱周向导波的传播特性

为研究无限大流体约束的孔隙圆柱中周向导波的传播规律,分析孔隙参数对导波传播特性的影响,建立了无限流体中孔隙介质圆柱的理论模型,利用孔隙介质弹性波动理论,建立了周向导波频散方程,通过数值模拟计算得到无限流体中孔隙介质圆柱的频散曲线,探讨了圆柱半径和孔隙参数对导波传播特性的影响,并对导波的衰减特性进行了分析;通过数值计算,得到了周向导波的时域波形,讨论了孔隙参数对波形的影响.结果表明,孔隙介质圆柱半径的改变影响圆柱尺度,孔隙度的改变影响孔隙介质中体声波的波速,都对周向导波频散曲线产生一定的影响,所得到的频散曲线特征及衰减曲线与时域波形吻合.研究结果对开展无限流体中孔隙介质圆柱的超声无损评价提供了一定的理论参考.     

Ultrasonic wave propagation in heterogeneous solid media: theoretical analysis and experimental validation

This research deals with the ultrasonic characterization of thermal damage in concrete. This damage leads to the appearance of microcracks which then evolve in terms of volume rate and size in the material. The scattering of ultrasonic waves from the inclusions is present in this type of medium. The propagation of the longitudinal wave in the heterogeneous media is studied via a homogenization model that integrates the multiple scattering of waves. The model allows us to determine the phase velocity and the attenuation according to the elements which make the medium. Simulations adapted to the concrete are developed in order to test the responses of the model. These behaviors are validated by an experimental study: the measurements of phase velocity and attenuation are performed in immersion, with a comparison method, on a frequency domain which ranges from 160 kHz to 1.3 MHz. The analysis of different theoretical and experimental results obtained on cement-based media leads to the model validation, on the phase velocity behavior, in the case of a damage simulated by expanded polystyrene spheres in granular media. The application to the case of a thermally damaged concrete shows a good qualitative agreement for the changes in velocity and attenuation.     

An investigation of the measurement of broadband ultrasonic attenuation in trabecular bone

Commercial devices for the ultrasonic characterisation of bone normally report the broadband ultrasonic attenuation (BUA). This is the slope of the attenuation against frequency in some part of the frequency range 200–1000 kHz. The assumption is that the relationship is linear and hence independent of the frequency range selected. In this study the ultrasonic attenuation in the frequency range 200 to 800 kHz was measured with a variety of transducers in ten trabecular heel bone samples from elderly cadavers, assumed to be osteoporotic.

The results indicate that the attenuation fits better to a second order polynomial function of frequency, than to the linear fit. The use of a straight line fit is only satisfactory in the higher frequency ranges (above 400 kHz). The use of lower frequencies results in a significant measurement error caused by the combination of a poor signal to noise ratio and the departure from linearity and this is greatest for samples with low attenuation. In the worst cases this can amount to a 30% discrepancy between the BUA values measured over different frequency ranges.     

非侵入式超声波浆料浓度测量技术研究*

设计了一种基于非侵入式超声波透射衰减法的浆料浓度测量系统,根据超声传播衰减原理,建立超声衰减值与浆料浓度之间的关系。实验中采用生物显微镜和激光粒度仪对颗粒标称粒径进行验证,采用中心频率为200 kHz的超声波换能器,利用一发一收模式对超声波在有机玻璃管内的浆料进行非侵入式测量并分析透射波信号,对体积百分浓度小于25%、不同粒径的石英砂浆料进行测量,通过拟合方法获得浆料温度、体积百分浓度与声衰减对应的关系,并据此构造浓度求解方程,通过现场实时在线测量并与取样结果进行对比验证方程的准确性,结果显示,本方法可有效测量浆料浓度。     

Damping rates of waves in a switched magnetoplasma medium:longitudinal propagation

The interaction of a circularly polarized electromagnetic wave with a switched-on magnetoplasma medium is considered. A static magnetic field in the direction of propagation is assumed to be present, resulting in longitudinal propagation. The incident wave splits into three waves whose frequencies are different from that of the incident wave. It is shown that these waves ultimately damp out if the plasma is even slightly lossy. The damping of the waves is interpreted in terms of their attenuation with distance and decay with time as they propagate in the lossy plasma. The attenuation-length and decay-time constants of the waves are obtained, and their dependence on the incident-wave frequency and the gyrofrequency is examined. Optimum parameters for an experiment to detect these waves are suggested     

Acoustic properties of multiferroic BiFeO<Subscript>3</Subscript> over the temperature range 4.2–830 K

The longitudinal acoustic wave velocity and attenuation in BiFeO₃ ceramics have been measured by ultrasonic pulse-echo technique at a frequency of 10 MHz in the temperature range from 4.2 K to 830 K. The anomalies observed in the sound velocity and attenuation behavior versus temperature are attributed to the assumed relaxation in the temperature range 200–500 K and antiferromagnetic phase transition at higher temperatures. Order parameter fluctuations along with magnetostriction are discussed as the factors determining the acoustic wave velocity anomaly in the vicinity of the antiferromagnetic phase transition point.     

Viscoelastic BISQ Model for Low-Permeability Sandstone with Clay

A modified BISQ （Blot/Squirt） model for wave propagation in low-permeability sandstone is developed by introducing the viscoelastic mechanism of a porous skeleton into Dvorkin＇s model. The linear viscoelasticity of the Kelvin Voigt constitutive law is employed to describe the stress-strain relation of a solid frame with clay while the ultrasonic waves propagate through the fluid-saturated sandstone. The phase velocity and attenuation of two p-waves are given based on the present BISQ model. The comparisons between numerical results and experimental data indicate that our viscoelastic model is more realistic and feasible for wave propagation in the low-permeability sandstone, especially with clay, than traditional BISQ models.