直位错和线性力作用下点群10十次对称二维准晶的弹性场研究

本文研究了直位错和线性力作用下点群10十次对称二维准晶的弹性场.首先将Stroh公式推广到点群10十次对称二维准晶研究中,在此基础上,采用推广的Stroh公式给出了应力和位移的通解,结合边界条件,获得了应力的解析表达式,为实际应用奠定了理论基础.     

十次对称二维准晶弹性半平面问题的复变函数方法

研究了集中力作用下二维十次对称准晶半平面弹性问题的复变函数方法.首先将Stroh公式推广到二维准晶中,这里保留了Stroh公式的本质特征,在此基础上,采用推广的Stroh公式给出了应力和位移的通解,结合边界条件,获得了应力和位移的解析表达式,为实际应用奠定了理论基础.表明复变函数方法是解决十次对称二维准晶复杂弹性边值问题的有力工具.     

一维纳米准晶层合梁的非局部振动、屈曲与弯曲研究

基于非局部理论,建立了一维纳米准晶层合简支深梁模型,研究了其自由振动、屈曲行为及其弯曲变形问题.采用伪Stroh型公式,导出了纳米梁的控制方程,并通过传递矩阵法获得简支边界条件下纳米准晶层合梁固有频率、临界屈曲载荷及弯曲变形广义位移和广义应力的精确解.通过数值算例,分析了高跨比、层厚比、叠层顺序及非局部效应对一维纳米准晶层合简支梁固有频率、临界屈曲载荷和弯曲变形的影响.结果表明：固有频率和临界屈曲载荷随着非局部参数增大而减小;外层准晶弹性常数更高时,固有频率和临界屈曲载荷更大;叠层顺序对纳米准晶梁的力学行为有较大影响.所得的精确解可为纳米尺度下梁结构的各种数值方法和实验结果提供参考.     

基于表面阻抗张量的界面滑移波动态失稳分析

基于Stroh公式和表面阻抗张量理论,提出了研究界面滑移波动态失稳问题的一种新的方法．该方法将表面阻抗张量概念推广到复波速域,并将摩擦接触界面上的边界条件以表面阻抗张量表示．最终将边值问题化归为求解一个复多项式在单位圆内的根．以弹性半空间与刚体平面相对稳态摩擦滑移为例进行了详细的分析,导出了一个4次复特征方程并讨论了方程在单位圆内解的特性,给出了滑移界面波失稳条件的显式解析表达式．     

一维六方准晶中带光滑顶点的正三角形孔边裂纹的反平面问题

本文通过引入合适的保角映射,利用Stroh公式和复变函数方法研究一维六方准晶材料中含光滑顶点的正三角形孔边裂纹的反平面问题,得到正三角形孔边裂纹尖端的场强度因子和能量释放率的表达式.通过数值算例,讨论了裂纹长度和正三角形孔口边长比值对等效场强度因子和能量释放率的影响,以及耦合系数和机械载荷对能量释放率的影响规律.结果表明:裂尖等效场强因子只与裂纹长度有关,而孔洞大小对其影响可忽略;裂纹长度、耦合系数和机械载荷总是促进裂纹扩展.     

Christoffel方程方法研究带有初应力压电介质中的表面波

利用Christoffel方程的方法研究了带有初应力的半无限大压电介质中的表面波.基于带有初应力的压电介质的控制方程和本构方程,构建带有初应力的Christoffel方程.再结合半空间应力自由的表面条件和电学的边界条件,得到了电学开路和电学短路时表面波的波速方程.这些结果可以为新型压电介质表面波器件的研究提供重要的理论依据.     

压电晶体表面任意源分布所产生的弹性波场

不久前,我们研究过在压电晶体表面一维源分布激发所产生的弹性波场。本文将推广到具有更普遍意义的二维任意源分布的激发问题。此时广义弹性波场是等于广义Green函数张量和广义力的双重点乘卷积。广义Green函数可以分别写成对应表面波、体波和静电效应三部分之和。利用二重积分的稳相方法,求得在远场的表面波和体波的渐近解,最后,举例进行了数值计算。     

反铁磁体表面空间磁孤子的频率特性 *

计及反铁磁晶体的非线性磁化效应,研究了反铁磁晶体中非线性TM表面波的传播特性.理论分析表明,在反铁磁界面上非线性TM表面波以空间磁孤子的形式传播,具有激发阈值.其场强峰值位置取决于材料与包层的相对折射率和导波的强度.表面空间磁孤子具有频率通带和禁带,带宽取决于导波频率、场强、晶体与包层的介电常数.通过调节表面波的功率可以实现通带和禁带的转换,预示了一种新型的非线性微波功率开关器件.     

表面效应对热电材料中纳米孔周围热应力的影响

基于完整Gurtin-Murdoch(G-M)低阶表面能模型，进一步探讨了纳米尺度下表面效应的影响.建立了合理考虑构型变化的应力边界条件，实现了研究尺度从宏观到微观的转变.利用复变函数理论和保角映射技术，构建了用于纳米尺度下的热-电-力理论框架模型，得到了热电基体中纳米孔周围热场、温度场以及应力场的半解析解.数值结果表明，相对于完整G-M模型，简化G-M模型(忽略孔洞构型变化的影响)往往会高估表面效应和远场热电载荷对热应力分布的影响.此外，表面效应的存在将在一定程度上缓解纳米孔周围的热应力集中.     

UPML吸收边界条件的无截断数值模拟

Berenger完全匹配层(PML)吸收边界条件完成了对非物理反射波的吸收,初步实现了有限区域对无限开放空间的数值模拟,然而在计算区域的边界上需要对场分量进行分裂,增加了Maxwell方程组中独立方程的个数,使场分量迭代复杂,增大了数值计算量,单轴各向异性完全匹配层(UPML)边界条件则不需要对场分量进行分裂,迭代公式简单,便于程序实现,且具有更好的宽频带吸收特性.首先推导了TMz波的UPML方程组,给出了UPML的介电参数分布方式,详细介绍了该算法的程序实现步骤,并以数值算例进行验证,分别采用常规PML和UPML边界条件进行数值计算,通过对比二者的计算结果,表明UPML边界条件具有更好的吸收效果,且能更有效地吸收低角入射波和低频凋落波,UPML边界条件更逼真地模拟了无限开放空间,更精确地实现了电磁波的无截断数值模拟.     

Surface waves in electrostrictive materials under biasing fields

The theory of small incremental fields superposed on finite biasing fields in an electroelastic body is summarized first in this paper. The Stroh formalism for two-dimensional anisotropic elasticity and piezoelectricity is generalized to two-dimensional problems of an electroelastic body under biasing mechanical and electric fields. Application of this generalized Stroh formalism to study surface waves propagating in an electroelastic half-space under uniform initial fields indicates that there exist at most two surface waves even in the presence of biasing fields and these two surface waves correspond to the well-known Rayleigh and Bleustein waves in the mechanical nature. A simple procedure is established to distinguish these two types of waves. Application of the results to a model electrostrictive material is included for illustration. It is found that initial biasing fields can greatly influence propagation feature of surface waves.     

Effect of phase-lags on Rayleigh wave propagation in initially stressed magneto-thermoelastic orthotropic medium

The present article deals with Rayleigh surface wave propagation in homogeneous magneto-thermoelastic orthotropic medium. Effect of initial stress and magnetic field on Rayleigh waves is studied in the context of three-phase-lag model of generalized thermoelasticity. The normal mode analysis is used to obtain the exact expressions for the displacement components, stresses and temperature distribution. Various frequency equations are derived and compared with the existing literature. The path of surface particles is elliptical during Rayleigh wave propagation. Effect of phase-lags on Rayleigh wave velocity, attenuation coefficient and specific loss are presented graphically. It is observed from graphical presentation that the effect of magnetic field and initial stress on different wave characteristics is pronounced.     

A generalized dynamic model of nanoscale surface acoustic wave sensors and its applications in Love wave propagation and shear-horizontal vibration

A generalized dynamic model to depict the wave propagation properties in surface acoustic wave nano-devices is established based on the Hamilton's principle and variational approach. The surface effect, equivalent to additional thin films, is included with the aid of the surface elasticity, surface piezoelectricity and surface permittivity. It is demonstrated that this generalized dynamic model can be reduced into some classical cases, suitable for macro-scale and nano-scale, if some specific assumptions are utilized. In numerical simulations, Love wave propagation in a typical surface acoustic wave device composed of a piezoelectric ceramic transducer film and an aluminum substrate, as well as the shear-horizontal vibration of a piezoelectric plate, is investigated consequently to qualitatively and quantitatively analyze the surface effect. Correspondingly, a critical thickness that distinguishes surface effect from macro-mechanical behaviors is proposed, below which the size-dependent properties must be considered. Not limited as Love waves, the theoretical model will provide us a useful mathematical tool to analyze surface effect in nano-devices, which can be easily extended to other type of waves, such as Bleustein-Gulyaev waves and general Rayleigh waves.     

An energy approach to the proof of the existence of Rayleigh waves in an anisotropic elastic half-space

An approach based on investigating the energy functional is applied for the first time to the classical problem of Rayleigh waves in an anisotropic half-space with a free boundary. The main object of the investigation is an ordinary differential operator in a variable characterizing the depth. An investigation of the spectrum by variational methods enables a new proof to be given of the existence of a Rayleigh wave in a linear elastic half-space with arbitrary anisotropy, which does not rest on the Stroh formalism.     

The effect of boundary conditions on the onset of chaos in Rayleigh–Bénard convection using energy-conserving Lorenz models

The influence of 16 boundary conditions on linear and nonlinear stability analyses of Rayleigh–Bénard system is reported. A Stuart–Landau amplitude equation for the Rayleigh–Bénard system between stress-free, isothermal boundary conditions is derived and the procedure used in this derivation serves as guidance for constructing an appropriate Fourier–Galerkin expansion for the other 15 boundary conditions to derive a generalized Lorenz model. The influence of the boundary conditions comes within the coefficients of the generalized Lorenz model. It is shown that the obtained generalized Lorenz model is energy conserving and for certain boundary conditions it retains features of the classical Lorenz model. Further, the principle of exchange of stabilities is shown to be valid for the present problem and hence it is the steady-state, linearized version of the generalized Lorenz model which yields an analytical expression for the Rayleigh number. On minimizing this expression with respect to wave number the critical Rayleigh number at which the onset of regular convective motion occurs in the form of rolls is determined for all 16 boundary conditions. It is found that these values are in good agreement with those of previous investigations leading to the conclusion that the chosen minimal Fourier–Galerkin expansion is a valid one. Exhibition of chaotic motion in the generalized Lorenz system at the Hopf Rayleigh number is studied. The phase-space plots which indicate a clear-cut visualization of the transition from regular convective motion to chaotic motion in the generalized Lorenz system are presented. Further, existence of a developing region for chaos (mildly chaotic motion) and windows of periodicity are captured using the bifurcation diagrams. It is concluded from the phase-space plots and the bifurcation diagrams that the generalized Lorenz model for certain sets of boundary conditions retains all the features of the classical Lorenz model. Such a conclusion cannot be made by a linear stability analysis and the need thus for a nonlinear analysis is highlighted in the paper.     

Propagation of Normal Waves in an Isolated Porous Fluid-Saturated Biot Layer

For a porous fluid-saturated Biot layer with boundaries free from stresses and pressure, the wave field is found and dispersion equations are derived. The roots of the dispersion equations and the dependence of the phase velocities of the normal waves on the wave number are investigated by analytic methods. It is shown that the phase velocities of most of the normal waves decrease with increasing wave number. Special investigations are conducted in the case of bend and plate waves and their phase velocities for high and low frequencies. It is also shown that on the boundary of a porous Biot half-space, the Rayleigh wave does not always originate, and conditions for the existence of such a wave are established. Bibliography: 7 titles.     

微极各向同性弹性板中的Rayleigh-Lamb波

研究了无应力作用条件下，均匀、各向同性、圆柱形微极结构弹性板中波的传播．导出了对称和斜对称模式下波传播的特征方程．对短波这一极端情况，无应力圆板中对称和斜对称模态波的特征方程退化为Pmyle曲表面波频率方程．并得到薄板的计算结果．给出了位移和微转动分量，并绘制了相应图形．给出了若干特殊情况的研究结果及对称和斜对称模态特征方程的图示．     

Surface waves in micropolar thermoelasticity

Free surface waves of arbitrary form in a homogeneous and isotropic linear micropolar thermoelastic half-space with stress-free plane boundary are investigated. It is found that all physical quantities associated with the waves are derivable from two scalar functions and that there exist two families of waves in general. One of these is the classical thermoelastic wave modified under the influence of the microelastic field and the other is a new surface wave not encountered in classical elasticity. The waves are not necessarily plane waves and even when these are assumed to propagate in a fixed direction parallel to the boundary, unlike in classical elasticity, the problem is not one of plane strain. Explicit expressions for the displacement vector, microrotation vector and the temperature are obtained and the nature of deformation has been analysed. Several earlier results are deduced as particular cases of the more general results obtained here.     

On interface waves in misoriented pre-stressed incompressible elastic solids

Some relationships, fundamental to the resolution of interfacewave problems, are presented. These equations allow for thederivation of explicit secular equations for problems involvingwaves localized near the plane boundary of anisotropic elastichalf-spaces, such as Rayleigh, Scholte, or Stoneley waves. Theyare obtained rapidly, without recourse to the Stroh formalism.As an application, the problems of Stoneley wave propagationand of interface stability for misaligned predeformed incompressiblehalfspaces are treated. The upper and lower half-spaces aremade of the same material, subject to the same prestress, andare rigidly bonded along a common principal plane. The principalaxes in this plane do not, however, coincide, and the wave propagationis studied in the direction of the bisectrix of the angle betweena principal axis of the upper half-space and a principal axisof the lower half-space.