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1.
Interaction between screw dislocations and a partially debonded interface in cylindrically anisotropic composites subjected
to uniform stress at infinity is investigated in this paper. Using Muskhelishvili’s complex variable method, the closed forms
of complex potentials are obtained for a screw dislocation and a screw dislocation dipole located inside either matrix or
inhomogeneity. Explicit expressions of stress intensity factors at the crack tips, image forces and image torques acting on
dislocation or the center of dipole are provided. The results show that the crack and dislocation geometry combination plays
an important role in the interaction between screw dislocations and interface crack. Furthermore, it is found that the anisotropy
of solids may change the shielding and anti-shielding effects arising from screw dislocations and the equilibrium position
of screw dislocations. The presented solutions are valid for anisotropic, orthotropic or isotropic composites and can be reduced
to some novel or previously known results. 相似文献
2.
The elastic interaction of screw dislocations and a star crack with a central hole was investigated. The complex potential of the present problem was obtained from that of an internal crack in an infinite medium using the conformal mapping technique. The stress field, image force and strain energy of dislocation, and stress intensity factor at the crack tip were derived. The critical stress intensity factor for dislocation emission was calculated based on the spontaneous dislocation emission criterion. The influence of the ratio of crack length to hole radius, crack number, and dislocation source on the above mechanical variables were studied. The present solution was reduced to several special cases previously reported in the literature. 相似文献
3.
该文研究了螺型位错偶极子和圆形夹杂界面裂纹的弹性干涉作用。利用复变函数方法,得到了该问题的复势函数以及应力场的封闭形式解答。求出了裂纹尖端的应力强度因子以及作用在螺型位错偶极子中心的像力和像力偶矩,并分析了位错偶极子对应力强度因子的影响及界面裂纹几何条件和不同材料特征组合对位错偶极子平衡位置的影响规律。研究结果表明:位错偶极子对应力强度因子具有很强的屏蔽或反屏蔽效应;硬夹杂排斥位错偶极子,而裂纹吸引位错偶极子,在一定条件下,位错偶极子在裂纹附近出现一个平衡位置;当裂纹的长度和材料剪切模量比达到临界值时,可以改变偶极子和界面之间的干涉机理。同时,裂纹长度对位错偶极子中心像力偶矩也有很大的影响。 相似文献
4.
The stress field around the tip of an elliptically blunted crack induced by an edge dislocation has been obtained in closed
form, from which the mode I and mode II stress intensity factors induced by the edge dislocation are obtained. The solutions
apply to the edge dislocation either emitted from crack-tip surface or originated elsewhere, and for the dislocation located
anywhere around the crack tip. The effects of the crack length, the crack-tip bluntness, the origination and position of the
dislocation on the stress intensity factors are examined. 相似文献
5.
A comparison of elastic interaction of a dislocation and a crack for four bonding conditions of the crack plane was made.
Four cases of single crystalline material, sliding grain boundary, perfectly bonded interface, and sliding interface were
considered. The stress intensity factors arising from edge and screw dislocations and their image forces for the above four
cases were compared. The stress intensity factor at a crack tip along the perfectly bonded interface arising from screw dislocation
can be obtained from that in a single crystalline material if the shear modulus in the single crystalline material is replaced
by the harmonic mean of both shear moduli in the bimaterial. The stress intensity factor at a crack tip along the sliding
interface arising from edge dislocation in the bimaterial can be obtained from that along the sliding grain boundary in the
single material if the μ/(1−ν) in the single material is substituted by the harmonic mean of μ/(1− ν) in the bimaterial where
μ and ν are the shear modulus and Poisson's ratio, respectively. The solutions of screw dislocation near a crack along the
sliding grain boundary and sliding interface are the same as that of screw dislocation and its mirror image. Generally, the
effect of edge dislocation for perfectly bonded interface on the crack propagation is more pronounced than that for the sliding
interface. The effect of edge dislocation on the crack propagation is mixed mode for the cases of perfectly bonded interface
and single crystalline material, but mode I fracture for the cases of sliding interface and sliding grain boundary. All curves
of Fx versus distance r from the dislocation at interface to the right-hand crack tip are similar to one another regardless
of dislocation source for both sliding interface and perfectly bonded interface. The level of Fx for m=0 is larger than that
for m=−1.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献
6.
7.
Calculation results to evaluate time variations of the stress intensity factor near the tip of the edge crack upon its stepwise growth are presented. The crack pop-in in a thick plate under tensile loading is shown to result in cyclic K
1 variations with a period and amplitude that are dependent on the initial crack length, pop-in length and plate dimensions. Time-average K
1 values correspond to those calculated for the stationary crack.__________Translated from Problemy Prochnosti, No. 2, pp. 66 – 71, March – April, 2005. 相似文献
8.
The dynamic field intensity factors and energy release rates in a piezoelectric ceramic block containing an edge crack with the condition of continuous electric crack faces under electromechanical impact loading are obtained. Integral transform method is used to reduce the problem to two pairs of dual integral equations, which are then expressed to an Fredholm integral equation of the second kind. Numerical values on the dynamic stress intensity factor and dynamic energy release rate are obtained to show the influence of the geometry and electric field. 相似文献
9.
Due to the singular behavior of the stress field near the interface edge of bonded dissimilar materials, fracture generally initiates near the interface edge, or just from the interface edge point. In this paper, an edge crack near the interface, which can be considered as being induced by the edge singularity and satisfying two conditions, is analyzed theoretically, based on the singular stress field near the interface edge and the superposition principle. It is found that the stress intensity factor can be expressed by the stress intensity coefficient of the edge singular stress field, the crack length, the distance between the interface and the crack, as well as the material combination. Boundary element method analysis is also carried out. It is found that the theoretical result coincides well with the numerical result when the crack length is small. Therefore, the theoretical representation obtained by this study can be used to simply evaluate the stress intensity factor of an edge singularity induced crack for this case. However, when the crack length becomes larger than a certain value, a significant difference appears, especially for the case with large edge singularity. 相似文献
10.
On contact zone models for an electrically impermeable interface crack in a piezoelectric bimaterial
An electrically impermeable interface crack between two semi-infinite piezoelectric planes under remote mechanical tension-shear and electrical loading is studied. Assuming the stresses, strains and displacements are independent on the coordinate x
2 the expressions for the elastic displacement and potential jumps as well as for the stresses and electrical displacement along the interface via a sectionally holomorphic vector function are found. Introducing an artificial contact zone at the right crack tip and assuming the materials possess the symmetry class 6 mm the problem is reduced for a wide range of bimaterial compounds to a combination of combined Dirichlet–Riemann and Hilbert boundary value problems which are solved analytically. From these solutions clear analytical expressions for characteristic mechanical and electrical parameters are derived. As particular cases of the above mentioned solution the classical (oscillating) and contact zone solutions are obtained. Further, a comparison with an associated solution for an electrically permeable crack has been performed. The fracture mechanical parameters for all models via the remote loads are found analytically and important relationships between these parameters are obtained. Due to these relationships an important algorithm of a numerical method applicable for the investigation of an interface crack in a finite sized piezoelectric bimaterial is suggested. 相似文献
11.
Avraham Dorogoy Leslie Banks‐Sills 《International journal for numerical methods in engineering》2004,59(13):1749-1780
Formulation of the elastic two‐dimensional problem of contact with friction is presented. Two‐dimensional equilibrium equations and boundary conditions in an orthogonal curvilinear co‐ordinate system are written explicitly. The above formulation is solved with the aid of the finite difference technique. An iterative algorithm which does not require load increments is employed for solving interface fracture problems with contact and friction subjected to a monotonically increasing load. The J‐integral is extended for problems in which there is friction along the crack faces. Stress intensity factors are calculated by means of the J‐integral, as well as an asymptotic expansion of the tangential shift. Two problems are analysed: (1) a crack in homogeneous material in the presence of friction involving stationary contact; and (2) an interface crack in the presence of friction involving receding contact. Results are compared to those found by analytical and semi‐analytical methods which are presented in the literature, as well as to those obtained by means of the finite element method. The accuracy of the results establishes the reliability of the finite difference analysis, as well as the post‐processors. In addition, a problem involving stick conditions is considered. It is observed that with increasing friction, the normal gaps and tangential shifts decrease. The size of the contact zone increases and values of the stress intensity factor decrease. Copyright © 2004 John Wiley & Sons, Ltd. 相似文献
12.
In this paper the stress intensity factors are discussed for an inclined elliptical crack near a bimaterial interface. The solution utilizes the body force method and requires Green’s functions for perfectly bonded semi-infinite bodies. The formulation leads to a system of hypersingular integral equation whose unknowns are three modes of crack opening displacements. In the numerical calculation, unknown body force densities are approximated by using fundamental density functions and polynomials. The results show that the present method yields smooth variations of stress intensity factors along the crack front accurately. Distributions of stress intensity factors are presented in tables and figures with varying the shape of crack, distance from the interface, and elastic modulus ratio. It is found that the inclined crack can be evaluated by the models of vertical and parallel cracks within the error of 24% even for the cracks very close to the interface. 相似文献
13.
The problem of finite bimaterial plates with an edge crack along the interface is studied. A complex variable boundary element
method is presented and applied to determine the stress intensity factor for finite bimaterial plates. Using the pseudo-orthogonal
characteristic of the eigenfunction expansion forms and the well-known Bueckner work conjugate integral and taking the different
complex potentials as auxiliary fields, the interfacial stress intensity factors associated with the physical stress-displacement
fields are evaluated. The effects of material properties and crack geometry on stress intensity factors are investigated.
The numerical examples for three typical specimens with six different combinations of the bimaterial are given.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
14.
Shicheng Zhang 《International Journal of Fracture》2000,106(3):277-290
The thermal stress intensities (energy release rate and stress intensity factors) due to temperature changes are derived in closed-form for an interface crack between two elastic layers of dissimilar materials. The solutions are two-dimensional and tabulated over a wide range of material and layer thickness combinations. The tables serve as rapid evaluations of the thermal stress intensities for given temperature changes. A strain gauge technique is given for determining constraint coefficients which reflect the constraint conditions during the temperature changes. The solutions are compared with results from the literature. The stress intensities due to thermal and mechanical loads are generally superimposed. As an example of application, the solutions are utilized to obtain the complete thermal and mechanical stress intensities for a four-point bend specimen. 相似文献
15.
F. Suat Kadioglu 《International Journal of Fracture》2002,116(1):51-79
In this paper, the axisymmetric elasticity problem of an infinitely long transversely isotropic solid cylinder imbedded in a transversely isotropic medium is considered. The cylinder contains an annular or a penny shaped crack subjected to uniform pressure on its surfaces. It is assumed that the cylinder is perfectly bonded to the medium. A singular integral equation of the first kind (whose unknown is the derivative of crack surface displacement) is derived by using Fourier and Hankel transforms. By performing an asymptotic analysis of the Fredholm kernel, the generalized Cauchy kernel associated with the case of `crack terminating at the interface' is derived. The stress singularity associated with this case is obtained. The singular integral equation is solved numerically for sample cases. Stress intensity factors are given for various crack geometries (internal annular and penny-shaped cracks, annular cracks and penny-shaped cracks terminating at the interface) for sample material pairs. 相似文献
16.
Weight functions proposed for interface cracks in dissimilar isotropic materials (Gao, 1991; Chen and Hasebe, 1994) are extended to treat those in piezoelectric materials. The difficulties in separating the eight distinct complex arguments are overcome. The pseudo-orthogonal properties of the eigenfunction expansion form found in isotropic dissimilar cases(Chen and Hasebe, 1994) are proved to be valid in the present cases although the mathematical manipulations performed here seem much more complicated than those in isotropic dissimilar materials. Several path-independent integrals are obtained and all the coefficients in the eigenfunction expansion form, including the K
I, K
II, K
III and K
e, could be calculated by the weight functions introduced in this paper. It is concluded that the weight functions presented here provide a powerful tool to calculate the dominant parameters at the interface crack tip without any special treatment to the singular stress field of the near-tip region. 相似文献
17.
C. B. Cui H. G. Beom H. S. Jang Q.‐Z. Fang H. M. Li 《Fatigue & Fracture of Engineering Materials & Structures》2013,36(10):968-980
We investigated the asymptotic problem of a kinked interface crack in an orthotropic bimaterial under in‐plane loading conditions. The stress intensity factors at the tip of the kinked interface crack are described in terms of the stress intensity factors of the interface crack prior to the kink combined with a dimensionless matrix function. Using a modified Stroh formalism and an orthotropy rescaling technique, the matrix function was obtained from the solutions of the corresponding problem in transformed bimaterial. The effects of orthotropic and bimaterial parameters on the matrix function were examined. A reduction in the number of dependent material parameters on the matrix function was made using the modified Stroh formalism. Moreover, the explicit dependence of one orthotropic parameter on the matrix function was determined using an orthotropic rescaling technique. The effects of the other material parameters on the matrix function were numerically examined. The energy release rate was obtained for a kinked interface crack in an orthotropic bimaterial. 相似文献
18.
Although a lot of interface crack problems were previously treated, few solutions are available under arbitrary material combinations. This paper deals with a central interface crack in a bonded finite plate and periodic interface cracks. Then, the effects of material combination and relative crack length on the stress intensity factors are discussed. A useful method to calculate the stress intensity factor of interface crack is presented with focusing on the stress at the crack tip calculated by the finite element method. 相似文献
19.
The undulant interface of a bi-material, which is due to manufacturing or instability under high stress, may provide certain preferred places where microdefects accumulate. In the present paper, an edge dislocation near a slightly wavy interface is studied via a regular perturbation scheme. Stress investigation for the interaction between the edge dislocation and the wavy bi-material interface has been carried out. The Peach-Koehler force on the dislocation is calculated from the first perturbed solution of the stress fields. The influence of several key parameters, such as the Dundurs bi-material interface constants α, β, the distance of the dislocation to the interface, the wavy extent of the interface, etc., on the behavior of the dislocation has been analyzed. The numerical examples indicate that there are certain “equilibrium” points around which the dislocations are expected to be accumulated. In turn, microdefects, such as microcracks and microvoids, may be initiated near these sites. Results obtained can be applied to study crack initiation or delamination along bonded bi-material interfaces. 相似文献
20.
Stress intensity factors for a kinked crack originating at interface of two bonded dissimilar materials subjected to normal
tension are found by the finite element method. 相似文献