共查询到16条相似文献,搜索用时 156 毫秒
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利用两相材料中集中力的基本解,建立了求解曲线型刚性线夹杂和两相材料界面相交问题的弱奇异积分方程。通过Cauchy型奇异积分方程主部分析方法,得出穿过两相材料界面的曲线型刚线性在交点处的奇性应力指数及交点处角形域内的奇性应力,并利用奇性应力定义了交点处的应力奇异因子。通过对弱奇异积分方程的数值求解,得出了刚性线端点和交点处的应力奇异因子。 相似文献
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折线型裂纹对SH波的动力响应 总被引:1,自引:0,他引:1
利用Fourier积分变换方法,得出了无限平面中用裂纹位错密度函数表示的单裂纹散射场.根据无穷积分的性质,把单裂纹的散射场分解为奇异部分和有界部分.利用单裂纹的散射场建立了折线裂纹在SH波作用下的Cauchy型奇异积分方程.根据折线裂纹散射场和所得的积分方程讨论了裂纹在折点处的奇性应力及折点处的奇性应力指数.利用所得的奇性应力定义了折点处的应力强度因子.对所得Cauchy型奇积分方程的数值求解,可得裂纹端点和折点处的动应力强度因子。 相似文献
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与两相材料界面接触的裂纹对SH波的散射 总被引:1,自引:0,他引:1
利用积分变换方法得出了两相材料中作用简谐集中力时的格林函数.根据所得的格林函数并利用Betti-Rayleigh互易定理得出了与界面接触裂纹的散射波场.裂纹的散射波场可分解为两部分,一部分为奇异的散射场,另一部分为有界的散射场.利用分解后的散射场,可得裂纹在SH波作用下的超奇异积分方程.根据裂纹散射场的奇异部分和Cauchy型奇异积分的性质得出了裂纹和界面接触点处的奇性应力指数和接触点角形域内的奇性应力.利用所得的奇性应力定义了裂纹和界面接触点处的动应力强度因子.对所得超奇异积分方程的数值求解可得裂纹端点和接解点处的应力强度因子。 相似文献
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利用双材料位移基本解和Somigliana公式,将三维体内含垂直于双材料界面混合型裂纹问题归结为求解一组超奇异积分方程。使用主部分析法,通过对裂纹前沿应力奇性的分析,得到用裂纹面位移间断表示的应力强度因子的计算公式,进而利用超奇异积分方程未知解的理论分析结果和有限部积分理论,给出了超奇异积分方程的数值求解方法。最后,对典型算例的应力强度因子做了计算,并讨论了应力强度因子数值结果的收敛性及其随各参数变化的规律。 相似文献
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研究两种材料界面上的刚性线与其它任意位置处直线裂纹弹性干涉的反平面问题。基于界面上刚性线与任意位置处螺型位错干涉的基本解,运用连续位错密度模型法将问题转化为奇异积分方程。用半开型积分法求解奇异积分方程,得到位错密度函数的离散值,计算裂纹尖端处的应力强度因子。算例说明该方法可用于工程实际问题。 相似文献
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对材料界面超高速自相似动态分层的反平面问题进行了解析分析。分层模拟为界面裂纹由零长度自相似扩展,扩展速度为蹭音速或超音速。首先考虑运动集中载荷作用下界面动态分层的情况,利用界面裂纹自相似扩展的运动位错模型将问题归结为奇异积分方程,并求得解析解,分析了裂纹尖端的应力奇性,获得了动应力强度因子。最后,利用叠加原理给出了x^n型载荷作用下界面动态分层的解。 相似文献
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The weakly singular integral equation used to solve the problem of the curved crack crossing the boundary of the antiplane
circular inclusion is presented. Using the principal part analysis method of the Cauchy type integral equation, the singular
stress index at the intersection and the singular stress of angular regions near the intersection are obtained. By using the
singular stress obtained, the stress intensity factor at the intersection is, defined. After the numerical solution of the
integral equation, the stress intensity factors at the end points of the crack and intersection are obtainable.
The research is supported by National Natural Science Foundation of China (No. 59879012) and is the project of Chinese Foundation
of State Education Commission (No. 98024832). 相似文献
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《International Journal of Solids and Structures》2003,40(13-14):3571-3588
The transient response of a piezoelectric strip with an eccentric crack normal to the strip boundaries under applied electromechanical impacts is considered. By using the Laplace transform, the mixed initial-boundary-value problem is reduced to triple series equations, then to a singular integral equation of the first kind by introducing an auxiliary function. The Lobatto–Chebyshev collocation technique is adopted to solve numerically the resulting singular integral equation. Dynamic field intensity factors and energy release rate are obtained for both a permeable crack and an impermeable crack. The effects of the crack position and the material properties on the dynamic stress intensity factor are examined and numerical results are presented graphically. 相似文献
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The interaction of a general plane P wave and an elastic cylindrical inclusion of infinite length partially debonded from
its surrounding viscoelastic matrix of infinite extension is investigated. The debonded region is modeled as an arc-shaped
interface crack between inclusion and matrix with non-contacting faces. With wave functions expansion and singular integral
equation technique, the interaction problem is reduced to a set of simultaneous singular integral equations of crack dislocation
density function. By analysis of the fundamental solution of the singular integral equation, it is found that dynamic stress
field at the crack tip is oscillatory singular, which is related to the frequency of incident wave. The singular integral
equations are solved numerically, and the crack open displacement and dynamic stress intensity factor are evaluated for various
incident angles and frequencies.
The project supported by the National Natural Science Foundation of China (19872002) and Climbing Foundation of Northern Jiaotong
University 相似文献
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The scattering of general SH plane wave by an interface crack between two dissimilar viscoelastic bodies is studied and the
dynamic stress intensity factor at the crack-tip is computed. The scattering problem can be decomposed into two problems:
one is the reflection and refraction problem of general SH plane waves at perfect interface (with no crack); another is the
scattering problem due to the existence of crack. For the first problem, the viscoelastic wave equation, displacement and
stress continuity conditions across the interface are used to obtain the shear stress distribution at the interface. For the
second problem, the integral transformation method is used to reduce the scattering problem into dual integral equations.
Then, the dual integral equations are transformed into the Cauchy singular integral equation of first kind by introduction
of the crack dislocation density function. Finally, the singular integral equation is solved by Kurtz's piecewise continuous
function method. As a consequence, the crack opening displacement and dynamic stress intensity factor are obtained. At the
end of the paper, a numerical example is given. The effects of incident angle, incident frequency and viscoelastic material
parameters are analyzed. It is found that there is a frequency region for viscoelastic material within which the viscoelastic
effects cannot be ignored.
This work was supported by the National Natural Science Foundation of China (No.19772064) and by the project of CAS KJ 951-1-20 相似文献
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Sei Ueda 《European Journal of Mechanics - A/Solids》2003,22(6):431-942
In this study, the dynamic response of a coated piezoelectric strip containing a crack vertical to the interfaces under normal impact load is considered. Based on the superposition principle and the integral transform techniques, the solution in the Laplace transformed plane is obtained in terms of a singular integral equation. The order of stress singularity around the tip of the terminated crack is also obtained. The singular integral equation is solved by using the Gauss–Jacobi integration formula, and the numerical Laplace inversion is then carried out to obtain the resulting dynamic stress and electric displacement intensities. The effects of the material properties and the geometric parameters on the dynamic stress intensity factor and the dynamic energy density factors are shown graphically. 相似文献