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1.
一个新的声应力系数及其确定   总被引:3,自引:0,他引:3  
 为建立声焦散线与平面应力条件下裂尖应力强度因子的关系,定义了一个新的声应力系 数------声程差随应力线性变化的比例系数, 该系数的大小既取决于材料常数又取决于 耦合介质及声束的传播历程. 借助6061-T6铝、EPTI钢两种材料的实验结果,说明了确 定新的声应力系数的方法与步骤. 所得结论是:只要确定了平面应力条件下超声纵波 速度相对变化与主应力和之比,便可确定新的声应力系数.  相似文献   

2.
为建立声焦散线与平面应力条件下裂尖应力强度因子的关系,定义了一个新的声应力系数——声程差随应力线性变化的比例系数,该系数的大小既取决于材料常数又取决于耦合介质及声束的传播历程.借助6061-T6铝、EPTI钢两种材料的实验结果,说明了确定新的声应力系数的方法与步骤.所得结论是:只要确定了平面应力条件下超声纵波速度相对变化与主应力和之比,便可确定新的声应力系数.  相似文献   

3.
声程差与应力强度因子的关系   总被引:2,自引:2,他引:0  
基于弹性状态下力对材料声折射率及试件厚度的影响,推导了含裂纹的试件受力前后,超声纵波经其前后表面反射及透射时声程的变化,得到了应力强度因子与声程差的关系,为通过声程差的变化确定裂尖应力强度因子打下了基础。  相似文献   

4.
使用焦散线法与光弹法测定三维裂纹混合型应力强度因子   总被引:1,自引:0,他引:1  
本文介绍了将焦散线法与应力冻结,“解冻”技术相结合,使焦散线法用于测量三维体内部裂纹前缘应力强度因子的实验方法,并针对复杂应力状态下三维裂纹前缘的不同应变奇异场,合理地综合运用焦散线法与三维光弹法,实际测量与分离了三维裂纹前缘混合型应力强度因子。  相似文献   

5.
本文介绍了一种测量应变奇异性的新方法-焦散线法。阐述了焦散线的基本理论和试验技术。得到了清晰的焦散线照相。材料的应力光学系数通过透射焦散线和反射焦散线的两尺寸比值来确定。通过试验,测定了单边裂纹板受拉时的应力强度因子,与计算结果附合良好。  相似文献   

6.
张忠平  王锋会 《力学季刊》2001,22(3):359-362
基于焦散线的形成原理及含裂纹受力试件在裂尖附近区域的应力分布,得到了焦散线法确定应力强度因子的条件:初始曲线半径与试件厚度之比大于0.5。当满足该条件时,对光学各向同性材料及光学各向异性材料前表面反射的情形,只需测量焦散线沿横向的最大尺寸便可较精确地确定应力强度因子;而对于光学各向异性材料的透射或后表面反射情形,只有在忽略远场非奇异应力的影响后,才可借助焦散线的横向尺寸近似确定应力强度因子。  相似文献   

7.
以光弹性法及焦散线法的基本原理为基础,对两种方法在确定应力强度因子方面进行了比较。发现对于纯I型裂纹问题,光弹性法的精度低于焦散线法的精度;对于I-Ⅱ混合型裂纹问题,就张开型应力强度因子而言,光弹性法的精度低于焦散线法的精度,而就滑移型应力强度因子而言,光弹性法的精度高于焦散线法的精度。  相似文献   

8.
本文介绍用激光焦散线法,测定中心的裂纹矩形板,在顺裂纹受压时的缝端应力强度因子的实验方法。与计算结果比较表明,结果吻合良好。 1 关于焦散线的基本关系激光焦散线法,是籍助于激光由高应变区所形成的曲面反射或透射时,因发散或汇聚所形成的干涉图,即焦散线,来研究应力强度因子,观测焦散线的光路如图1,其中参数为本实验所采用的。  相似文献   

9.
管大椿  金江 《实验力学》1996,11(4):457-462
为提高焦散线法求解应力强度因子的精度,提出了两种基于多点非线性最小二乘法的改进方法。文中推导了控制方程,编制了程序,阐述了实验技术。作为应用实例,对三种典型裂纹试件作了测试与处理。结果表明,用本文方法处理的结果比文[1]经典法的结果有很大改进。作者还对图像处理用于焦散线法应力强度因子的提取作了初步探讨[5  相似文献   

10.
唐巨鹏  齐桐  代树红  路江伟 《应用力学学报》2020,(3):990-998+1385-1386
为揭示地应力环境对周期注水应力改造提高压裂效果的影响规律,以黑龙江双鸭山矿区煤系页岩为研究对象,克服煤系页岩非均质性,利用相似比制作型页岩试件,开展了实验室真三轴水力压裂试验。利用声发射技术监测裂缝起裂和扩展特征,通过RA-AF散点分布特征给出了应力改造和压裂阶段主导裂缝类型,分析得到了周期注水应力改造下水平地应力差对裂缝特征以及裂缝起裂、扩展的影响规律,提出了起裂阶段与扩展阶段声发射判断指标。试验结果表明:应力改造阶段裂缝起裂与扩展以微裂缝为主,剪切型微裂缝占比波动上升,第2个周期裂缝主频范围最大,裂缝发育最为活跃;压裂阶段裂缝起裂与扩展以宏观裂缝为主,张拉型裂缝占比呈增加趋势,当水平地应力差与注水压力接近2.0MPa时,张拉型裂缝占比最大,分布范围最广,压裂效果最显著。另外,本文提出了裂缝起裂与扩展阶段声发射判断指标为平均声发射能率k。k降幅在37.74%以上时,裂缝由起裂阶段进入扩展阶段。周期注水应力改造可以减小水平地应力差对裂缝扩展的约束能力,促进微裂缝大量发育、沟通天然裂缝形成缝网,从而提高页岩气开采率。  相似文献   

11.
动态裂纹扩展中的分形效应   总被引:20,自引:0,他引:20  
谢和平 《力学学报》1995,27(1):18-27
假设裂纹顶端沿着分形轨迹运动,建立了裂纹扩展的分形弯折(kinking)模型来描述裂纹的动态扩展。根据这个模型,我们推导了分形裂纹扩展对劝态应力强度和裂纹速度的影响.动态应力强度因子与表观应力强度因子之比K(l(t),V)/K(L(t),O)是表观裂纹速度V_O,材料微结构参数(d/Δa),分维D和裂纹扩展路径的弯折角θ的函数。本文研究结果表明:在分形裂纹扩展中,表观(或量测)的裂纹速度V_O很难接近Rayleigh波速C_r.动态断裂实验中V_O明显低于C_r的原因可能是分形裂纹扩展效应所致。材料的微结构,裂纹扩展路径的分维和弯折角均很强地影响动态应力强度因子和裂纹扩展速度。  相似文献   

12.
In this work we investigate the stability of a nominally straight two-dimensional quasistatically growing crack to a small perturbation of its path. Formulae for perturbations of stress intensity factors induced by slight deviation of the crack trajectory were developed by Movchan et al. (Int. J. Solids Struct. 35, 3419) Their solution is exploited to derive an equation for the perturbation of the crack path on the assumption that the crack advances in pure “opening” mode (i.e. local KII=0). Various types of loading conditions are considered, including a cracked body loaded by a pair of point body forces and a crack whose faces are subjected to given tractions acting in the direction normal to the crack boundary. The body is also subjected to a remotely maintained uniaxial stress, aligned with the direction of the unperturbed crack. The loading is assumed to advance as the crack advances, to maintain the critical value of Mode I stress intensity factor. Numerical computations of possible crack paths have been performed, extending results on crack stability obtained by Cotterell and Rice (Int. J. Fract. 16, 155). The results show that in the case of loading by point body forces the stability of the crack path depends on the positions of the points of application of the applied forces and the magnitude of the applied stress acting parallel to the crack. There exists a critical value of this stress such that the crack path is stable for values less than critical and unstable otherwise. It is shown that the crack is always unstable in the case of point force tractions applied normal to the crack faces.  相似文献   

13.
弯曲载荷作用下,双槽圆形截面管的角裂纹具有两个不同的奇异应力场和相应的应力强度因子,针对该异型薄壁管裂纹问题,提出了一种简单实用的应力强度因子求解方法。即利用守恒律,通过选取适当的三维积分路径,并结合初等力学的应力位移计算方法,显化了应力强度因子对J_2积分的贡献,建立了一个求解应力强度因子的方程。由于该方程不足以求解两个应力强度因子,利用材料力学平截面保持平面的变形假设,建立了应力强度因子之间的补充方程。将J_2积分与补充方程联立求解,既可得到弯曲载荷作用下双槽圆形截面管角裂纹的应力强度因子。对于其他异型薄壁管裂纹问题,该方法同样适用,计算过程简单。  相似文献   

14.
The variation of stress field around an oscillating crack tip in a quenched thin glass plate is observed using instantaneous phase-stepping photoelasticity. The successive images around the propagating crack are recorded by a CCD camera that is equipped with a pixelated micro-retarder array. Then, the phase maps of the principal stress difference and the principal direction are easily obtained even though the photoelastic fringes cannot be visualized. The path of the crack growth as well as the stress intensity factors and the crack tip constraint are obtained from these phase distributions. Results show that the mode I stress intensity factor and the crack tip constraint vary remarkably with the crack growth. In addition, the results show that the mode-II stress intensity factor exists even though the crack propagates smoothly.  相似文献   

15.
轮轨滚动接触下,钢轨表面会产生典型的鱼钩形剥离掉块,其形成机理目前暂未明确.为了探究轮轨滚动接触下钢轨表面裂纹扩展机理,基于最大周向拉应力准则,建立轮轨滚动接触疲劳计算模型,提出裂尖扩展路径预测方法,并对不同初始角度裂纹的扩展路径进行预测.结果表明,钢轨表面微裂纹为Ⅰ-Ⅱ复合型裂纹,随着裂纹长度增加,KⅠ先增加后减小,...  相似文献   

16.
We present a new method for determining the elasto-dynamic stress fields associated with the propagation of anti-plane kinked or branched cracks. Our approach allows the exact calculation of the corresponding dynamic stress intensity factors. The latter are very important quantities in dynamic brittle fracture mechanics, since they determine the crack path and eventual branching instabilities. As a first illustration, we consider a semi-infinite anti-plane straight crack, initially propagating at a given time-dependent velocity, that changes instantaneously both its direction and its speed of propagation. We will give the explicit dependence of the stress intensity factor just after kinking as a function of the stress intensity factor just before kinking, the kinking angle and the instantaneous velocity of the crack tip.  相似文献   

17.
Mixed-Mode Dynamic Crack Growth in Functionally Graded Glass-Filled Epoxy   总被引:5,自引:0,他引:5  
Compositionally graded glass-filled epoxy sheets with edge cracks initially along the gradient are studied under dynamic loading conditions. Specimens with monotonically varying volume fraction of reinforcement are subjected to mixed-mode loading by eccentric impact relative to the crack plane. The optical method of Coherent Gradient Sensing and high-speed photography are used to map transient crack tip deformations before and after crack initiation. Two configurations, one with a crack on the stiffer side of a graded sheet and the second with a crack on the compliant side, are examined experimentally. To elucidate the differences in fracture behavior due to functional grading, a homogeneous sample is also tested. The differences in both pre- and post-crack initiation behaviors are observed interms of crack initiation time, crack path, crack speed and stress intensity factor histories. When a crack is situated on the compliant side of the sample, it kinks significantly less compared to when it is on the stiffer side. Crack tip mode mixity histories show small but positive values during crack growth from the stiffer side of the sample towards the compliant side whereas a small but negative mode mixity prevails for the opposite configuration.  相似文献   

18.
In this paper, the dynamic crack-interface interactions and the related mechanics of crack penetration vs. branching at a weak interface are studied experimentally. The interface is oriented perpendicular to the incoming mode-I crack in an otherwise homogeneous bilayer. The focus of this investigation is on the effect of interface location and the associated crack-tip parameters within the bilayer on the mechanics of the ensuing fracture behavior based on the optical methodologies laid down in Ref. Sundaram and Tippur (2016). Time-resolved optical measurement of crack-tip deformations, velocity and stress intensity factor histories in different bilayer configurations is performed using Digital Gradient Sensing (DGS) technique in conjunction with high-speed photography. The results show that the crack path selection at the interface and subsequently the second layer are greatly affected by the location of the interface within the geometry. Using optically measured fracture parameters, the mechanics of crack penetration and branching are explained. Counter to the intuition, a dynamically growing mode-I approaching a weak interface at a lower velocity and stress intensity factor penetrates the interface whereas a higher velocity and stress intensity factor counterpart gets trapped by the interface producing branched daughter cracks until they kink out into the next layer. An interesting empirical observation based on measured crack-tip parameters for crack penetration and branching is also made.  相似文献   

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