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1.
本文采用考虑裂纹面上具有任意分布载荷的线弹簧模型,在Kirchhoff板弯曲理论的假设下,将含半椭圆型表面裂纹的平板问题化为一组耦合的积分方程组进行求解,对均匀拉伸和纯弯曲两种载荷作用下的应力强度因子数值解,同经典线弹簧模型和有限元解进行了比较,并给出了经典线弹簧模型不能得到的、裂纹面上承受幂次不均匀应力分布时应力强度因子的数值解.  相似文献   

2.
无限平板内埋裂纹线弹簧模型   总被引:9,自引:1,他引:8  
建立了无限平板内埋椭圆形裂纹的弹簧模型,用积分变换方法推导了问题的控制积分方程笔应力强度因子的表达式,给出了数值结果,并与现有交替迭代解进行了比较,结果表明模型的应用是合理的。  相似文献   

3.
现存文献关于梯度材料断裂问题的研究大都是假设材料参数为坐标的指数函数或幂函数,而其它函数形式较少采用.本文假设功能梯度材料剪切模量和密度的倒数均为坐标的线性函数,而泊松比为常量,研究功能梯度板条的反平面运动裂纹问题.利用Fourier积分变换技术和传递矩阵法将混合边值问题化为一对奇异积分方程,通过数值求解奇异积分方程获得板条运动裂纹在反平面载荷作用下的动态应力强度因子,并讨论了裂纹运动速度、裂纹相对尺寸、以及材料非均匀性对动态应力强度因子的影响,结果证明梯度参数、裂纹速度和几何尺寸对材料动态断裂行为有显著影响.  相似文献   

4.
柴国钟  洪起超 《力学学报》1999,31(4):498-503
鉴于用通常的数值方法分析三维蠕变裂纹问题的困难,提出了一个三维表面裂纹蠕变断裂力学参量分析的蠕变线弹簧模型方法,并在非稳态蠕变条件下的位移、裂纹尖端J积分和C积分的工程估算公式及弹塑性线弹簧模型的基础上,建立了蠕变线弹簧模型方法的有关基本方程.具体分析计算了受均匀拉伸表面裂纹平板的J积分和C积分,并与三维有限元解进行了比较,其结果吻合良好.研究结果为进一步研究三维表面裂纹的蠕变扩展及寿命预报提供了基础.  相似文献   

5.
采用线弹簧模型求解含焊接残余应力平板多个共面任意分布表面裂纹的应力强度因子.利用边裂纹权函数给出了裂纹表面上沿厚度非线性分布的残余应力向线性分布的转化公式.基于Reissner板理论和连续分布位错思想,将含多个共面任意分布表面裂纹的无限平板问题归结为一组Cauchy型奇异积分方程,并采用Gauss-Chebyshev方法获得了奇异积分方程的数值解.以三共面表面裂纹为例,计算了表面裂纹的应力强度因子,并讨论了裂纹间距、裂纹几何形状等因素对应力强度因子的影响.  相似文献   

6.
本文由Reissner型板的不连续位移基本解,根据Betti互换定理,导出了Reissuer型板的不连续位移边界积分方程;结合平面问题的不连续位移边界积分方程─—边界元方法和线弹簧模型,给出了Rrissner型板表面裂纹应力强度因子的线弹簧-不连续位移边界积分方程解法。  相似文献   

7.
功能梯度板条断裂分析   总被引:2,自引:0,他引:2  
程站起  仲政 《力学季刊》2005,26(4):544-548
现存文献关于功能梯度材料断裂问题的研究大都假设材料性质为坐标的指数函数或幂函数,而对其它函数形式较少采用。本文假设功能梯度材料剪切模量为坐标的双曲函数,而泊松比为常量,研究功能梯度板条的混合型裂纹问题。利用Fourier积分变换技术将混合边值问题转化为一对奇异积分方程,通过数值求解奇异积分方程获得含裂纹功能梯度板条分别在剪切和法向载荷作用下的I型和Ⅱ型应力强度因子,并讨论了材料的非均匀性和裂纹相对尺寸对裂纹尖端应力强度因子的影响。  相似文献   

8.
本文采用分解D-M模型,然后利用设形式函数的方法和Abel 积分方程法求解Fourier 积分变换解中心裂纹问题中的对偶积分方程,严格而又比较简单地求得了D-M 模型的COD、CTOD 以及裂纹线上的σ_(?)(x,0)  相似文献   

9.
本文采用分解D-M模型,然后利用设形式函数的方法和Abel 积分方程法求解Fourier 积分变换解中心裂纹问题中的对偶积分方程,严格而又比较简单地求得了D-M 模型的COD、CTOD 以及裂纹线上的σ_(?)(x,0) ...  相似文献   

10.
本文由Reissner型板的不连续位移基本解,根据Betti互换定理,导出了Reissner型板的不连续位移边界积分方程,结合平面问题的不连续位移边界积分方程--边界元方法和线弹簧模型,给出了Reissner型板表面裂纹应力强度因子的线弹簧-不连续位移边界积分方程解法。  相似文献   

11.
The mechanical model was established for the anti-plane dynamic fracture problem for two collinear cracks on the two sides of and perpendicular to a weak-discontinuous interface between two materials with smoothly graded elastic properties, as opposed to a sharp interface with discontinuously changing elastic properties. The problem was reduced as a system of Cauchy singular integral equations of the first kind by Laplace and Fourier integral transforms. The integral equations were solved by Erdogan's collocation method and the dynamic stress intensity factors in the time domain were obtained through Laplace numerical inversion proposed by Miller and Guy. The influences of geometrical and physical parameters on the dynamic stress intensity factors were illustrated and discussed, based on which some conclusions were drawn: (a) to increase the thickness of the FGM strip on either side of the interface will be beneficial to reducing the DSIF of a crack perpendicular to a bi-FGM interface and embedded at the center of one of the FGM strips; (b) To increase the rigidity of the FGM strip where the crack is located will increase the DSIF. However, when the material in one side of the interface is more rigid, the DSIF of the interface-perpendicular embedded crack in the other side will be reduced; (c) To decrease the weak-discontinuity of a bi-FGM interface will not necessarily reduce the stress intensity factor of a crack perpendicular to it, which is different from the case of interfacial crack; (d) For two collinear cracks with equal half-length, when the distance between the two inner tips is less than about three times of the half-length, the interaction of them is intensified, however, when the distance is greater than this the interaction becomes weak.  相似文献   

12.
建立并研究一类接触型界面裂纹模型对瞬态弹性波作用下的动态响应问题。文中利用积分变换和积分方程法推导了确定这类问题的奇异积分方程组。采用围道积分技术和切比雪夫多项式展开技术,得到了待定系数的非线性代数方程组。最后给出了裂纹尖端接触区大小和接触应力随时间变化的数值结果,揭示了这种接触裂纹的动力学特性及物理上的合理性。  相似文献   

13.
The dynamic theory of antiplane piezoelectricity is applied to solve the problem of a line crack subjected to horizontally polarized shear waves in an arbitrary direction. The problem is formulated by means of integral transforms and reduced to the solution of a Fredholm integral equation of the second kind. The path-independent integral G is extended here to include piezoelectric effects, and is evaluated at the crack tip to obtain the dynamic energy release rate. Numerical calculations are carried out for the dynamic stress intensity factor and energy release rate. The material is piezoelectric ceramic.  相似文献   

14.
给出了一组只包含Cauchy主值积分、不含有强奇异积分的三维静动力边界积分方程及其应用于裂纹问题的具体列式,并给出了几何轴对称问题的相应半解析边界元求解方法,将三维问题降阶为一维数值问题.文中分析了无限、半无限介质中圆裂纹、平行圆裂纹系、球面裂纹等在静载及应力波作用下的静力或瞬态动力响应问题,求得了相应的应力强度因子.  相似文献   

15.
SH波对内含裂纹衬砌结构的散射及动应力集中   总被引:2,自引:0,他引:2  
当衬砌结构内含裂纹时 ,采用Green函数的方法 ,研究了SH波对裂纹的散射及其动应力集中 ,构造了在含有半圆形衬砌的弹性半空间上 ,在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 ;推导了SH波对衬砌内有裂纹的散射定解积分方程组 ,进而求得裂纹尖端的动应力因子 ,重点讨论了衬砌及周围介质对裂纹尖端动应力因子的影响 ,给出了介质参数变化对裂纹尖端动应力因子的影响曲线 ,为工程设计提供了依据。  相似文献   

16.
We study dynamic antiplane cracks in the time domain by the boundary integral equation method (BIEM) based on the integral equation for displacement discontinuity (or crack opening displacement, COD) as a function of stress on the crack. This displacement discontinuity formulation presents the advantage, with respect to methods developed by Das and others in seismology, that it has to be solved only inside the crack. This BIEM is, however, difficult to implement numerically because of the hypersingularity of the kernel of the integral equation. Hence it is rewritten into a weakly singular form using a regularization technique proposed by Bonnet. The first step, following a method due to Sladek and Sladek, consists in converting the hypersingular integral equation for the displacement discontinuity into an integral equation for the displacement discontinuity and its tangential derivatives (dislocation density distribution); the latter involves a Cauchy type singular kernel. The second step is based on the observation that the hypersingularity is related to the static component of the kernel; the static singularity is then isolated and can be expressed in terms of weakly singular integrals using a result due to Bonnet. Although numerical applications discussed in this paper are all for the antiplane problem, the technique can be applied as well to in-plane crack dynamics.

The BIEM is implemented numerically using continuous linear space-time base functions to model the COD on the crack. In the present scheme the COD gradient interpolation is discontinuous at the element nodes while the integral equations are collocated at the element midpoints. This leads to an overdetermined discrete problem which is solved by standard least-squares methods. We use the dynamic BIEM to study a set of problems that appear in earthquake source dynamics, including the spontaneous dynamic crack propagation for a very simple rupture criterion. The numerical results compare favorably with the few exact solutions that are available. Then we demonstrate that difficulties experienced with finite difference simulations of spontaneous crack dynamics can be removed with the use of BIEM. The results are improved by the use of singular crack tip elements.  相似文献   


17.
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   

18.
多个共面任意分布表面裂纹的应力强度因子   总被引:2,自引:0,他引:2  
采用线弹簧模型求解多个共面任意分布表面裂纹的应力强度因子。基于Reissner板理论和连续分布位错思想,通过积分变换方法,将含有多个共面任意分布表面裂纹的无限平板问题归结为一组Cauchy型奇异积分方程。利用Gauss-Ghebyshev笔法获得了奇异积分方程的数值解。为验证本文法的正确性,文中最后给出了有关应力强度因子或P-V曲线的数值结果并与现有的理论结果或实验结果进行了对比。结果表明了连续位  相似文献   

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