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本文求解了一个圆形夹杂物对裂纹尖端应力场的影响,计算了反平面切变问题经典的应力场和应力强度因数,进而求得了非局域应力场,得到非奇异的裂纹尖端应力的解析表达式,讨论了解的应用。
关键词: 相似文献
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利用无限介质中的格林函数,本文首先导出一般形状的夹杂所产生的拘束应力场,夹杂中的无应力应变εij*可以是位置的函数,在此基础上,给出了平面问题的全部计算公式,文中把裂纹或空腔看做是其弹性常数为零的一种特殊的异性夹杂,在物体受到外加应力场的作用时,计算了与椭圆空腔等效的夹杂的无应力应变,对于扁平形状的夹杂,在其端点附近显示出与裂纹完全类似的r-1/2式应力奇点,算出了相应的应力强度因子,对于本文结果的一些应用做了讨论,例如椭圆空腔与外加应力场的交互作用,马氏体转变和形变孪晶所伴随形成的微观裂纹等。
关键词: 相似文献
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通过分子动力学方法模拟了三维 α-Fe I型裂纹的单向拉伸实验中的裂纹扩展过程。研究了在不同温度下裂纹扩展时位错的形成过程和断裂机理。计算结果表明,裂纹扩展过程是位错不断发射的过程。 裂纹尖端附近先形成无位错区和层错,当裂纹处应力增加到KI=0.566 MPam1/2时,裂纹尖端附近的某一层原子会逐渐分叉形成两层原子,分层后的原子层继续分离形成位错;当应力KI 达到0.669MPam1/2时第一个位错发射。随着温度的升高,临界应力强度因子逐渐降低,同时位错发射也相应地加快。 相似文献
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通过分子动力学方法模拟了三维 α-Fe I型裂纹的单向拉伸实验中的裂纹扩展过程。研究了在不同温度下裂纹扩展时位错的形成过程和断裂机理。计算结果表明,裂纹扩展过程是位错不断发射的过程。 裂纹尖端附近先形成无位错区和层错,当裂纹处应力增加到KI=0.566 MPam1/2时,裂纹尖端附近的某一层原子会逐渐分叉形成两层原子,分层后的原子层继续分离形成位错;当应力KI 达到0.669MPam1/2时第一个位错发射。随着温度的升高,临界应力强度因子逐渐降低,同时位错发射也相应地加快。 相似文献
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为从理论上揭示钛金属应力腐蚀行为的本质,建立了α钛晶粒及位错塞积形成的微裂纹原子 集团模型,利用递归法(recursion)计算了裂纹及晶粒内的电子结构参量(费米能级、结构能 、表面能、团簇能、环境敏感镶嵌能). 计算结果表明:氢在裂纹处的环境敏感镶嵌能较低 ,易于偏聚在裂纹处,且氢在钛金属裂纹处团簇能为正值不能形成团簇,具有有序化倾向, 趋于形成氢化物. 氢在裂纹处偏聚降低裂纹的表面能,使裂纹容易扩展. 裂纹尖端处费米能 级高于裂纹其他区域,使电子从裂纹尖端流向裂纹其他区域造成电位差,在电解质作用下裂
关键词:
递归法
电子结构
钛
应力腐蚀 相似文献
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利用热弹性理论分析了在光学材料中由于缺陷吸收激光能量引起的温度和热应力分布,并且针对一个简单的裂纹模型分析了热应力产生的应力强度因子,并且给出了一些主要参数对于应力强度因子的影响的规律。 相似文献
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《Journal of Physics and Chemistry of Solids》1987,48(11):1007-1014
In this paper, recent developments in the understanding of the dislocation-crack interaction and its relationship to the phenomena of crack tip deformation and fracture toughness are reviewed. An enhanced research activity in this area began with successful observations of the behavior of crack tip dislocations by various techniques, namely etch pits technique, X-ray topography and transmision electron microscopy. The advantages and limitations of these techniques are compared and the information obtained from these experiments are discussed. The results show that dislocations are emitted from a crack tip when the applied stress is sufficiently high. During crack propagation, dislocations are also generated from other bulk sources and the number of these dislocations relative to those from the crack tip may be an important parameter. The elastic theory of the interaction between dislocations and a crack is presented by considering the force on the dislocations. The theory is applied to derive a dislocation emission condition, which may be expressed in terms of a critical stress intensity factor. It is concluded that the dislocations emitted from a crack tip are repelled from the crack tip and this repulsive interaction is responsible for the formation of a dislocation-free zone. These dislocations shield the crack tip from the applied stress and hence contribute to an increase in the fracture toughness. The physical origin of the dislocation-free zone lies in the presence of a barrier to dislocation emission from the crack tip. One of the barriers to dislocation emission is the image stress. With the dislocation-free zone, the crack tip can maintain a finite stress intensity factor following crack tip deformation. The lattice theories of dislocation-crack interaction indicate that the results are consistent with those of the continuum theory. 相似文献
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Based on the displacement potential functions, the elastic analysis
of a mode II crack in an icosahedral quasicrystal is performed by
using the Fourier transform and dual integral equation theory. By the
solution, the analytic expressions for the displacement field and
stress field are obtained. The asymptotic behaviours of the phonon
and phason stress fields around the crack tip indicate that the
stresses near the crack tip exhibit a square root singularity. The
most important physical quantities of fracture theory, crack stress
intensity factor and energy release rate, are evaluated in an
explicit version. 相似文献
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The evolution of the distribution of interstitial impurity atoms in the plastic zone around the tip of a tension crack is
analyzed. The transport of point defects is determined by: 1) the hydrostatic component of the elastic stress at the crack
tip, created by the superposition of the elastic fields of the crack and dislocations; 2) the elastic field of moving dislocations
(“sweeping out” of interstitial impurity atoms); 3) the dislocation-driven transport of point defects present in the dislocation
cores. The contributions of each mechanism of transport of point defects to the crack tip are calculated over the entire time
from the start of loading of a sample containing a crack until an equilibrium distribution of plastic deformation is established
after the cessation of loading. Numerical calculations are carried out for interstitial hydrogen atoms dissolved in an α-Fe crystal.
Fiz. Tverd. Tela (St. Petersburg) 39, 1580–1585 (September 1997) 相似文献
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Shielding effect and emission criterion of a screw dislocation near an interfacial blunt crack
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Shielding effect and emission criterion of a screw dislocation near
an interfacial blunt crack are dealt with in this paper. Utilizing
the conformal mapping technique, the closed-form solutions are
derived for complex potentials and stress fields due to a screw
dislocation located near the interfacial blunt crack. The stress
intensity factor on the crack tips and the critical stress intensity
factor for dislocation emission are also calculated. The influence
of the orientation of the dislocation and the morphology of the
blunt crack as well as the material elastic dissimilarity on the
shielding effect and the emission criterion is discussed in detail.
The results show that positive screw dislocations can reduce the
stress intensity factor of the interfacial blunt crack tip
(shielding effect). The shielding effect increases with the increase
of the shear modulus of the lower half-plane, but it decreases with
the increase of the dislocation azimuth angle. The critical loads at
infinity for dislocation emission increases with the increase of
emission angle and curvature radius of blunt crack tip, and the most
probable angle for screw dislocation emission is zero. The present
solutions contain previous results as special cases. 相似文献
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Abstract The problem of a Belt chamber matrix cracking is presented. The influence of crack surface quality on the effective values of near crack tip stress is discussed. It is shown that under working conditions of the vessel, the existing shear friction between upper and lower crack surfaces caused by crack surface roughness can prevent the crack surface sliding displacement. Therefore, the control variable for matrix cracking is the value of stress intensity factor KI corresponding to normal node of loading only. The calculations are performed by finite element method within the range of linear elastic fracture mechanics. 相似文献
16.
Elastic behaviour of an edge dislocation near a sharp crack emanating from a semi-elliptical blunt crack
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The interaction between an edge dislocation and a crack
emanating from a semi-elliptic hole is dealt with. Utilizing the
complex variable method, closed form solutions are derived for
complex potentials and stress fields. The stress intensity factor at
the tip of the crack and the image force acting on the edge
dislocation are also calculated. The influence of the morphology of
the blunt crack and the position of the edge dislocation on the
shielding effect to the crack and the image force is examined in
detail. The results indicate that the shielding or anti-shielding
effect to the stress intensity factor increases acutely when the
dislocation approaches the tip of the crack. The effect of the
morphology of the blunt crack on the stress intensity factor of the
crack and the image force is very significant. 相似文献
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This paper gives a quantitative analysis of the effect of near-tip microcracks on electric-field-induced stress intensity factors in isotropic elastic dielectrics. Nucleation of the microcracks is assumed to be governed by the electric-field-induced mean stress or the maximum normal stress. Based on the solutions for the effect of a single microcrack on the local electric field at the main crack, simple formulae are derived for the electric-field-induced stress intensity factors in the presence of the microcracks. It is found that the relative change in the stress intensity factor due to the microcracks for a conducting crack is equal and opposite to that for an insulating crack provided that the distribution of microcrack orientations is random. In particular, the microcracking zone is found to amplify the electric-field-induced stress intensity factor in some cases, especially for stationary insulating cracks, while the microcracking zone wake has an antishielding effect for sufficiently grown conducting cracks. These results are in sharp contrast with the well-known toughening effects of microcracks in elastic media under pure mechanical loads. This is attributed to the fact that the interaction between the microcracks and the main crack in elastic dielectrics under electrical loading is governed essentially by electrostatics, while the shape of the microcracking zone is determined by the electric field induced elastic stress field. 相似文献
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G.A. Papadopoulos 《Optics and Lasers in Engineering》1990,13(3-4):211-249
For the study of elastodynamic problems of propagating cracks it is necessary to evaluate the dynamic stress intensity factor KdI which depends on the form of expressions for the stress components existing at the running crack tip at any instant of the propagation of the crack and the corresponding dynamic mechanical and optical properties of the material of the specimen under identical loading conditions. In this paper the distortion of the form of the corresponding reflected caustic from the lateral faces of a dynamically loaded transparent and optically inert specimen containing a transverse crack running under constant velocity was studied on the basis of complex potential elasticity theory and the influence of this form on the value of the dynamic stress intensity factor was given. The method was applied to the study of a propagating Mode I crack in a PMMA specimen under various propagation velocities and the corresponding dynamic stress intensity factor KdI evaluated. Also, crack propagation behaviour of notched composites in dynamic loading modes are reviewed and evaluated. A relatively large data base using metal-epoxy particulates, rubber-toughened poly(methyl methacrylate), and Sandwich plates are given. In all cases, a combination of high-speed photography and the optical method of dynamic caustics has been used. Results on the dynamic crack propagation mode, fracture toughness and crack propagation velocities of several rubber-modified composite models are presented. The composite models studied include specimens with one and/or two ‘complex’ two-stage inclusions, i.e. PMMA round inclusions surrounded by concentric rubber rings, one and/or press-fifting inclusions without rubber interface, all under dynamic loading. In all cases both qualitative and quantitative results were obtained. Also, results on crack propagation mode, crack propagation velocity, stress intensity factors and on the influence of the sandwich phases on crack propagation mode are presented. 相似文献