SH波在界面孔上散射的远场解

采用Green函数和复变函数方法研究了界面上任意形柱状孔洞对SH波散射的远场解。取含有任意形凹陷的弹性半空间,在其水平表面上任意一点承受时间谐和的反平面线源荷载作用时的位移解作为Green函数,按"契合"的方式构造出两种不同介质交界面上任意形孔洞对SH波的散射模型,利用Green函数建立求解问题的第一类Fredholm积分方程组,求解散射波的远场位移模式和散射截面。通过算例,分析了不同材料组合情况下界面椭圆孔和方孔对SH波散射的远场特性。     

海底沉积层中高阶界面波对多掩埋物散射分析

根据界面波散射迭代公式,并利用含多个异质体弹性动力学的散射积分方程,引出海底沉积层中界面波高阶模式对掩埋物的散射情况。根据建立的分层海底模型,对沉积层中传播的界面波进行模式分解。利用界面波传播的Green函数构建界面波散射迭代积分,并根据弹性波对多异质体散射理论,将界面波散射积分推广到对多目标的散射情况。由模式分解的结果,求解出了前三阶界面波对多目标的散射情况,并对界面波高阶模式传播及对不同目标的散射情况做了分析。     

SH 波对圆形夹杂与裂纹的散射及其动应力集中

采用Green 函数的方法, 研究了介质中同时存在夹杂与裂纹时对SH 波的散射, 构造了在含有半圆形夹杂的弹性半空间, 水平面上任一点承受时间谐和出平面线源载荷作用时的位移函数作为Green 函数。并推导了SH 波对夹杂与裂纹散射的定解积分方程组, 进而求得裂纹尖端的动应力因子。重点讨论了夹杂的存在对裂纹尖端动应力因子的影响, 给出了随夹杂介质参数及夹杂与裂纹距离对裂纹尖端动应力因子的分布曲线, 为工程设计提供参考依据。　      

加层压电层硬币型裂纹断裂分析

研究粘接着弹性层的压电层内硬币型裂纹的断裂问题。压电层与弹性层均为横观各向同性材料,r轴方向无限长,z轴方向有限厚度。压电层沿z轴方向极化。考虑电不导通裂纹表面条件,利用Hankel积分变换将问题化为求解积分方程组,导出了场强度因子与能量释放率的表达式。给出了数值计算结果,并分析了弹性层厚度对场强度因子与能量释放率的影响。     

弹性波在横向受限的固态声子晶体中的传输特性

对横向受限的一维固态声子晶体，得出了弹性波在其中传输时的模式数所满足的条件，并利用多层介质的转移矩阵计算了纵波入射时，不同模式下透射波的透射系数随弹性波频率变化的特点：出现声子禁带；不同模式的禁带宽度并不完全相同。横波入射时中心频率以下全为禁带，1倍中心频率以下没有透射峰出现。     

非均匀弹簧界面模型下柱形夹杂物对弹性波的散射

利用波函数展开法研究了非均匀弹簧界面模型(弹簧系数沿周向非均匀分布)下单个柱形夹杂物对弹性波的散射问题。在弹簧界面模型中,当弹簧系数沿周向分布均匀时,可利用波函数的正交性简化边界条件;当弹簧系数沿周向分布不均匀时,不能利用波函数的正交性简化边界条件。该文研究了这一问题,通过沿周向的离散化将弹性波散射的边界条件归结为一个超定线性代数方程组。针对Ge-Al纤维增强复合材料数值计算了散射截面和远场散射幅。特别地,通过适当选取弹簧常数的周向分布处理了含裂纹界面的弹性波散射问题,数值计算了裂纹张开位移和错开位移。     

脉冲源反演介质参数的近似波前法

在时域内对弹性波动方程退化的非均匀介质声波方程，引入背景场参数与扰动参数，并化为积分方程形式；针对脉冲源情况，根据射线理论中的传递方程和程函方程，对非均匀介质中的波场形式引入一种波前近似形式，得到波散射点满足散射关系曲线及散射波幅值与介质参数扰动比的代数关系方程式；为求解非均匀介质中散射波场及反演介质参数提供了一种方法，通过对一个完整算例全部过程的模拟，验证了此方法的正确性。     

双相介质界面附近裂纹的断裂力学特征

复合材料界面附近的力学性态对于材料的性能和强韧化影响是非常重要的。首先研究和讨论了含裂纹的双相介质的J 积分守恒定律的适用性问题, 采用有限元法证明了当裂纹平行靠近界面时, 其J 积分数值与裂纹位置无关的假设。文中建立了一种双相介质界面附近存在斜裂纹的分析模型, 用有限元和数值拟合相结合的方法, 得到了在远场单轴拉应力作用下, 斜裂纹处在不同介质中, 近界面一端裂尖的é 型能量释放率近似计算公式, 和相应的应力强度因子的计算方法。     

双相介质中椭圆孔洞与裂纹对SH波的散射

采用Green函数法和保角映射法解答了双相介质界面附近一个椭圆孔洞和一个裂纹(在同一侧)对SH波的散射问题。沿水平界面将双相介质剖分为一个含椭圆孔和裂纹的半空间以及一个完整的弹性半空间。结合“裂纹切割”法,利用Green函数法构造裂纹,求解出孔洞与裂纹同时存在时的位移和应力表达式。一组未知力系施加在水平界面上,使两部分契合,基于界面连续条件推导出一系列Fredholm积分方程组,从而求出未知力系。最后,给出算例讨论了不同参数对椭圆孔周边动应力集中系数和裂纹尖端动应力强度因子的影响。     

弹性波三维散射快速多极子间接边界元法求解

边界元方法对于无限域中弹性波散射求解具有独特优势,但求解矩阵的非对称稠密特征极大限制了该方法在大规模实际工程中的应用。为此,基于单层位势理论,结合快速多极子展开技术,通过对球面压缩波和剪切波势函数的泰勒级数展开,建立一种新的快速多极间接边界元方法,以实现大规模弹性波三维散射的精确高效模拟。算例分析表明所提方法能够大幅度降低计算时间和存储量,可在目前普通计算机上快速实现上百万自由度弹性波三维散射问题的快速精确求解。最后以全空间椭球形孔洞群对平面P波、SV波的散射为例,揭示了三维孔洞群周围稳态位移场和应力场的若干分布规律。该文方法对低无量纲频率（ka<5.0）的大规模多体散射问题尤为适合。     

Elastodynamics of a crack on the bimaterial interface

The paper is an application of boundary integral equations to the problem of a crack located on the bimaterial interface under time-harmonic loading. A system of linear algebraic equations is derived for solving the problem numerically. The distributions of the displacements and tractions at the bimaterial interface are obtained and analysed for the case of a penny-shaped crack under normal tension-compression wave. The dynamic stress intensity factors (normal and shear modes) are also computed. The results are compared with those obtained for the static case.     

Time-domain boundary element analysis of elastic wave interaction with a crack

The mathematical formulation of the problem of transient wave interaction with a crack in a homogeneous, isotropic, linearly elastic solid has been reduced to the solution of an integral equation over the insonified crack face. The integral equation relates the unknown crack-opening displacement, which depends on time and position, to the incident wave field. The integral equation has been solved numerically by a time-stepping method in conjunction with a boundary element discretization of the crack surface. For normal incidence of a longitudinal step-stress wave on a penny-shaped crack, results as functions of time have been obtained for the crack-opening displacement, the elastodynamic Mode-I stress intensity factor and the scattered far-field.     

The effect of internal pressure on a penny-shaped crack at the interface of two bonded dissimilar micropolar elastic half-spaces

In the linear theory of micropolar elasticity, the problem of a penny-shaped crack at the interface of two bonded dissimilar micropolar elastic half spaces is studied. The problem is first reduced to a system of dual integral equations which are further reduced to the solution of Riemann-Hilbert problem. Further stresses at the rims of cracks and in the vicinity have been evaluated.     

Scattering of inhomogeneous wave by viscoelastic interface crack

Summary The reflection, refraction and scattering of inhomogeneous plane waves of SH type by an interface crack between two dissimilar viscoelastic bodies are investigated. The singular integral equation method is used to reduce the scattering problem into the Cauchy singular integral equation of first kind by introduction of the crack dislocation density function. Then, the singular integral equation is solved numerically by Kurtz's piecewise continous function method. The crack opening displacement and dynamic stress intensity factor characterizing the scattered near-field are estimated for various incident angles, frequencies and relaxation times. The differences on crack opening displacement and stress intensity factor between elastic and viscoelastic interface crack are contrasted. And the effects of incident angle, incident frequency and relaxation time of the viscoelastic material are analyzed and explained by the features of phase lag and energy dissipation of the viscoelastic wave.     

The contact problem for an open penny-shaped crack under normally incident tension-compression wave

This paper concerns fracture dynamic problems for elastic cracked solids with allowance for crack faces contact interaction. The contact problem for a penny-shaped crack with an initial opening under normally incident tension-compression wave is solved by the method of boundary integral equations. The contact forces and the displacement discontinuity of the crack faces are studied. The solution is compared with those obtained without allowance for crack faces contact interaction for various shapes of the initial opening.     

A magneto-electro-elastic material with a penny-shaped crack subjected to temperature loading

Summary The analysis of intensity factors for a penny-shaped crack under thermal, mechanical, electrical and magnetic boundary conditions becomes a very important topic in fracture mechanics. An exact solution is derived for the problem of a penny-shaped crack in a magneto-electro-thermo-elastic material in a temperature field. The problem is analyzed within the framework of the theory of linear magneto-electro-thermo-elasticity. The coupling features of transversely isotropic magneto-electro-thermo-elastic solids are governed by a system of partial differential equations with respect to the elastic displacements, the electric potential, the magnetic potential and the temperature field. The heat conduction equation and equilibrium equations for an infinite magneto-electro-thermo-elastic media are solved by means of the Hankel integral transform. The mathematical formulations for the crack conditions are derived as a set of dual integral equations, which, in turn, are reduced to Abel's integral equation. Solution of Abel's integral equation is applied to derive the elastic, electric and magnetic fields as well as field intensity factors. The intensity factors of thermal stress, electric displacement and magnetic induction are derived explicitly for approximate (impermeable or permeable) and exact (a notch of finite thickness crack) conditions. Due to its explicitness, the solution is remarkable and should be of great interest in the magneto-electro-thermo-elastic material analysis and design.     

Penny-shaped interface crack between dissimilar nonhomogeneous elastic layers under axially symmetric torsion

Summary The problem of axially symmetric torsion for dissimilar nonhomogeneous bonded elastic layers containing a penny-shaped interface crack is considered. The mixed boundary value problem is reduced to solving a Fredholm integral equation of the second kind. The Fredholm integral equation is solved numerically by reducing it to a system of simultaneous algebraic equations. Numerical results for the stress intensity factor are presented in the form of graphs.     

The interface penny-shaped crack reconsidered

The penny-shaped crack at the interface between two bonded dissimilar media is reconsidered on the basis of recent developments on the elimination of oscillatory singularities. This is accomplished by assuming an annular frictionless contact zone at the crack circumference and reducing the problem to a Fredholm integral equation. Expressions for the strain energy, crack opening force and bond stresses are obtained and numerical results given for specific material combinations.     

On interface crack propagation with variable velocity for longitudinal shear problems

The antiplane strain problem of straight interface crack propagation between two elastic half-spaces under arbitrary variable loading is considered. The crack edge is specified as an arbitrary smooth function of time. It is assumed that the crack speed is less than the smaller of the shear wave velocities of two media. An integral transform method and factorization technique are used to solve the problem. The solutions are worked out for semi-infinite crack and finite crack problems. The dynamic stress intensity factors at the crack tip of the moving interface crack are given and it is found that the stress intensity factor of the interface crack is slightly higher than that in the homogeneous medium with slower shear wave velocity.