用超声透射频谱方法定征金属板的弹性常数

本文采用超声双透射技术测量了水中各向同性金属板的超声透射频谱，将透射频谱的理论值与实验值实现最佳拟合，具体反演得到了金属板的杨氏模量和泊松比。     

超声脉冲背向散射法测量悬浊液浓度的研究

本文报导了在不同浓度和不同粒径的水泥浆悬浊液中超声脉冲背向散射讯号的数字特征,主要是幅域和频域特征.对于不同的浓度范围,可以取不同的背向散射讯号特征量(如散射声强或散的衰减)来表征是浊液的浓度和粒径.对于低浓度范围,相对散射声强与浓度有较好的线性关系,对于高浓度范围,声强的散射衰减与浓度有较好的线性关系,高浓度与低浓度之间存在着过渡区域,在此区域内,散射声强随浓度的增加与散射衰减随浓度的增加呈动态平衡,因而在过渡区域内散射声强将与浓度无关,并与频率或粒径有关,当频率一定时,可确定粒径分布.     

考虑界面状况时柱状弹性固体的声波散射

导出了求解母材料固体中镶嵌的柱状弹性固体(两固体间存在界面薄层)声波散射系数的一般表达式.根据Flax的共振散射理论,对背向散射谱中的共振模式进行了识别.利用模拟界面薄层的弹簧模型,考察了界面层切向劲度常数K_T对共振模式形态的影响 关键词： 声波散射 共振模式 界面     

柱状分层固体媒质的声散射

本文评述了各向同性和横向各向同性柱状分层固体声散射理论和实验研究进展介绍了描述圆柱状界面薄层特性的弹簧模型，也讨论了该领域中有待进一步研究的一些问题。     

共振非弹性X射线散射——一种新型的X射线谱学探测方法的介绍

文章对一种新型X射线谱学探测方法——“共振非弹性X射线散射”进行了介绍,对它的方法特点和优势以及在各个领域内的最新研究进展做了简要概括.     

共振非弹性X射线散射——一种新型的X射线谱学探测方法的介绍

文章对一种新型X射线谱学探测方法——"共振非弹性X射线散射"进行了介绍,对它的方法特点和优势以及在各个领域内的最新研究进展做了简要概括.     

单向复合纤维材料弹性系数的超声测量

本文将单向复合纤维材料视作六角对称晶体，认为其弹性特征由五个独立的弹性系数来描述。利用Christoffel方程，我们得到这一各向异性介质中不同方向的声波速度与弹性系数的关系．我们还建立了一套计算机控制的实验测量系统，通过它对纤维板样品中的声速进行测量，反演得到了五个独立的弹性系数C11、C33、C13、C14和C12。理论计算得到的声速和实验测量值吻合较好，表明我们的方法是有实用意义的。     

Temperature dependence of elastic constants for ionic solids

In this paper the thermal variation of volume for NaCl, KCl, MgO and CaO has been investigated on the basis of Anderson model. We have evaluated the values of elastic constants C₁₁, C₄₄ and K_T at different temperature on the basis of Murnaghan and Tallon models. Tallon's model with second approximation presents slightly better agreement with experimental results which shows that the Anderson–Grüneisen parameter is directly proportional to the volume ratio. Tallon's model can be used to evaluate the values of elastic constants for solids at different temperatures.     

Temperature variation of higher-order elastic constants of MgO

An effort has been made for obtaining higher-order elastic constants for MgO starting from basic parameters, viz. nearest-neighbor distance and hardness parameter using Coulomb and Börn-Mayer potentials. These are calculated in a wide temperature range (100–1000 K) and compared with available theoretical and experimental results.     

Anomalies in second order elastic constants and gyrotropic constants of triglycine sulphate near phase transition

The anomalies in second order elastic constants and gyrotropic constants have been considered for the phase transition of triglycine sulphate. Expressions have been derived for the equilibrium values of order parameter and strain variables in both phases. Using Landau-Khalatnikov equation the fluctuation in order parameter is expressed in terms of fluctuations in strain variables. Substitution of these in free energy gives anomalies arising from Landau and coupling energies in second order elastic constants. The real part of the anomalies decreases steeply across the transition temperature and thereafter flatly tend to ferroelectric values. The anomalies in the components of the gyrotropic tensor have been derived and their temperature variation discussed.     

High pressure phase transitions and variation of elastic constants of some II-VI semiconductors

This paper reports an investigation of the pressure-induced phase transitions and dependence of elastic constants of ZnS, ZnSe and ZnTe on pressure using a three-body-potential (TBP) approach. The phase-transition pressures and associated volume collapses obtained from this approach show a reasonably good agreement with experimental data. The variations of elastic constants and their combinations with pressure follow a systematic trend, identical to that observed in other semiconductors of the zincblende structure family. It is found that this TBP model has a promise to predict the phase-transition pressure and the pressure variation of elastic constants of other semiconductors as well.     

Higher-order elastic constants of La1.84Sr0.16CuO4 high-temperature superconductor

Finite deformation theory is used to obtain the strain energy density of a tetragonal 2–1–4-type single crystal of the high-temperature superconductor La_2−xSr_xCuO₄. The complete set of second and third-order elastic constants of the high-temperature superconductor La_2−xSr_xCuO₄ (x = 0.16) is calculated by taking into account the interactions between nine nearest-neighbour atoms in the lattice and using Mie–Grüneisen interatomic potential. For the sake of comparison we have also computed the values of these constants for x = 0.13–0.20. The values of third-order elastic constants of La_2−xSr_xCuO₄ (x = 0.13–0.20) are negative and their absolute magnitudes are one order higher than those of the second-order elastic constants.     

Pseudo-molecular approach for the elastic constants of nematic liquid crystals interacting via anisotropic dispersion forces

The bulk and the surface-like elastic constants of a nematic liquid crystal are calculated for an ensemble of particles interacting via anisotropic dispersion forces using the pseudo-molecular method. The geometrical anisotropy of the molecules is also taken into account in the calculations by choosing a molecular volume of ellipsoidal shape. Analytical expressions for the elastic constants are obtained as a function of the eccentricity in the molecular volume shape. The method allows one to explore the dependence on the molecular orientation with respect to the intermolecular vector by analyzing the magnitude and the behaviour of macroscopic elastic parameters defining the nematic phase.     

Elastic constants of solids and fluids with initial pressure via a unified approach based on equations-of-state

The second and third-order Brugger elastic constants are obtained for liquids and ideal gases having an initial hydrostatic pressure p₁. For liquids the second-order elastic constants are C₁₁ = A + p₁, C₁₂ = A − p₁, and the third-order constants are C₁₁₁ = −(B + 5A + 3p₁), C₁₁₂ = −(B + A − p₁), and C₁₂₃ = A − B − p₁, where A and B are the Beyer expansion coefficients in the liquid equation of state. For ideal gases the second-order constants are C₁₁ = p₁γ + p₁, C₁₂ = p₁γ − p₁, and the third-order constants are C₁₁₁ = −p₁(γ² + 4γ + 3), C₁₁₂ = −p₁(γ² − 1), and C₁₂₃ = −p₁ (γ² − 2γ + 1), where γ is the ratio of specific heats. The inequality of C₁₁ and C₁₂ results in a nonzero shear constant C₄₄ = (1/2)(C₁₁ − C₁₂) = p₁ for both liquids and gases. For water at standard temperature and pressure the ratio of terms p₁/A contributing to the second-order constants is approximately 4.3 × 10⁻⁵. For atmospheric gases the ratio of corresponding terms is approximately 0.7. Analytical expressions that include initial stresses are derived for the material ‘nonlinearity parameters’ associated with harmonic generation and acoustoelasticity for fluids and solids of arbitrary crystal symmetry. The expressions are used to validate the relationships for the elastic constants of fluids.     

基于频域幅度谱数据重建电磁脉冲时域波形

 由频域幅度谱数据重建时域脉冲波形，是电磁脉冲效应及传感器标定研究中经常遇到的问题。根据最小相位原理，利用倒谱技术，编程实现了从频域幅度谱数据构造相位信息，进而反演时域脉冲响应波形。对几类函数波形和一组实测高空核爆电磁脉冲(HEMP)波形的验证结果表明，HEMP波形、余(正)弦阻尼振荡波形等信号的重建波形与原始波形符合很好。对于非最小相位信号，重建波形的前(后)沿、峰值等细节参数有一定差别，但也能给出一些波形、累积能量、幅值量级等方面的标志信息。