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1.
针对评价复合材料层合板层间断裂韧性的测量,提出了用拉伸试验法测定Ⅱ型层间断裂韧性,设计了内含铺层拼接区的分层破坏试验层合板,制备了拉伸试件.通过拉伸试验测得了拼接区开裂和分层裂纹稳态扩展过程中的载荷与变形规律:层间破坏具有Ⅱ型断裂特征,且裂纹扩展比较稳定.利用测试数据计算出断裂功,并以临界能量释放率表示层合板的Ⅱ型层间断裂韧性,结果表明用铺层拼接件拉伸法进行层间断裂韧性试验是可行的.  相似文献   

2.
从经典梁理论和弹性基础上的正交各向异性梁理论出发,分析了梁的弯曲剪切效应和弹性基础对用双悬臂梁试件测得的复合材料层合板Ⅰ型层间断裂韧性G_(IC)的影响,发现当试件的初始裂纹长度较短时,剪切效应和弹性基础对G_(IC)的影响是显著的,建议将初始裂纹长度取50毫米。实验结果表明,初始裂纹长度由20毫米增加到50毫米时,测得的G_(IC)值的离散系数降低20%~40%,数据趋于稳定,分散性减小。  相似文献   

3.
本文依据裂纹沿渗碳层扩张时所特有的POP-in现象提出了一种评定渗碳层断裂韧性的新方法。研究表明:POP-in现象是渗碳层断裂韧性正梯度分布造成的;根据POP-in点处的载荷及相应的裂纹长度计算出的渗碳层KIC-x分布曲线是评定其断裂韧性的基础,而对渗碳层断裂韧性的客观评定需综合考虑断裂韧性沿渗层的分布及梯度分布  相似文献   

4.
基于短纤维增强金属基复合材料的单纤维轴对称和三维细观力学模型,利用弹塑性有限元分析方法对该复合材料中基体与纤维间的应力传递进行研究,研究中主要讨论了基体、纤维和界面的力学性能以及纤维位向的变化对应力传递和应力分布的影响。研究表明,复合材料微结构参数的变化将显著影响基体与纤维间的应力传递和复合材料中的应力分布,复合材料设计过程中必须考虑合理的微结构特征。  相似文献   

5.
纤维-基体界面剪切强度与断裂韧性的表征和测定   总被引:1,自引:0,他引:1  
根据单向复合材料纤维分布、剪切变形与裂纹扩展的细观分析,提出纤维-基体界面剪切强度和断裂韧性的简易细观表征与测定方法.  相似文献   

6.
根据单向复合材料纤维分布、剪切变形与裂纹扩展的细观分析,提出纤维一基体界面剪切强度和断裂韧性的简易细观表征与测定方法.  相似文献   

7.
根据单向复合材料纤维分布、剪切变形与裂纹扩展的细观分析,提出纤维一基体界面剪切强度和断裂韧性的简易细观表征与测定方法.  相似文献   

8.
对石英纤维布增强氰酸酯树脂基复合材料进行了常温、低温和湿热三种环境下的拉伸、压缩、面内剪切、层间剪切和钉孔挤压等试验研究,得到了该复合材料的拉伸压缩面内剪切的强度和弹性模量以及层间剪切强度和钉孔挤压强度等力学性能参数。结果表明:石英纤维布增强氰酸酯树脂基复合材料的力学性能参数具有温度相关性。在低温环境下,力学性能参数不同程度地增强,最大增长量达40%;而在高温环境下,力学性能参数则明显下降,最高下降量达到56%。另外,由于复合材料的层间性能主要由基体决定,所以湿热环境对复合材料层间性能的影响很大,在工程实际中应特别关注。  相似文献   

9.
本文采用三维有限元模型,对典型铺设的[0_2/±45_2/90_2]_s碳/环氧复合材料层板中分层伴以横向裂纹的产生和扩展导致的层间应力分布进行了分析。计算结果表明层间裂纹首先在90°层中部出现并开裂至相邻界面处而产生横向裂纹,横向裂纹的出现引起局部分层按三角形状扩展;并指出分层损伤过程是一个主导性的稳定扩展过程,这是导致刚度下降的主要因素。最后,数值计算结果与实验结果比较,两者是吻合的。  相似文献   

10.
本文将长距离显微云纹干涉方法与显微放大技术相结合,在轴向拉伸载荷下,对AS4/PEEK[0/±45/90]2S层合板层间变形、纤维-基体脱粘和基体裂纹进行了从小变形到大变形直至分层损伤的全过程实时、定量的细观变形测量分析.实验表明:AS4/PEEK[0/±45/90]2S层合板亚临界损伤的主要特征,是中间90°/90°层基体中出现具有一定间隔的基体裂纹群.初步探讨了热塑性复合材料AS4/PEEK层合板基体的非弹性变形和损伤过程的一些基本特征.  相似文献   

11.
李俊  冯伟哲  高效伟 《力学学报》2016,48(2):387-398
相对于有限元法,边界单元法在求解断裂问题上有着独特的优势,现有的边界单元法中主要有子区域法和双边界积分方程法.采用一种改进的双边界积分方程法求解二维、三维断裂问题的应力强度因子,对非裂纹边界采用传统的位移边界积分方程,只需对裂纹面中的一面采用面力边界积分方程,并以裂纹间断位移为未知量直接用于计算应力强度因子.采用一种高阶奇异积分的直接法计算面力边界积分方程中的超强奇异积分;对于裂纹尖端单元,提供了三种不同形式的间断位移插值函数,采用两点公式计算应力强度因子.给出了多个具体的算例,与现存的精确解或参考解对比,可得到高精度的计算结果.   相似文献   

12.

2008年5月12日,汶川M80地震在四川省绵竹市清平乡文家沟内诱发一巨型滑坡。通过现场调查得知,滑坡前后缘高差455m,厚度20~30m,滑面为基岩层面,初始方量2750×107m3。滑体在运动中转化为碎屑流。滑坡-碎屑流总的水平运动距离为4022m,垂直运动距离为1443m,遗留的堆积物体积达5×107m3。滑坡距映秀—北川断裂仅36km,位于其下盘,地震烈度达XI度。滑坡导致文家沟中48人遇害,并形成一条完整的地震次生地质灾害链。初步分析表明滑坡启动速度快,滑坡向碎屑流转化过程明显、地点明确。碎屑流运动过程复杂,伴有强烈的“气垫效应”和“前缘气浪冲击效应”。作者认为,文家沟滑坡的高启动速度是长持时强烈地震动作用的结果,与山体的猛烈碰撞是导致滑体解体并转化为碎屑流的原因。  相似文献   

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16.
One of the core issues in modern celestial mechanics is the orbital dynamics in the near-regime gravitational field of as- teroids, which provides deep insights into the mathematical nature of a class of nonlinear systems, and plays as a critical basis for in situ explorations of different science goals. Lots of efforts have been made to reveal the characteristics of orbital motion in the vicinity of asteroids, and to improve the skills of asteroid research in methodology.  相似文献   

17.
Experimental studies of the plasticity mechanisms of polycrystals are usually based on the Schmid factor distribution supposing crystalline elasticity isotropy. A numerical evaluation of the effect of crystalline elasticity anisotropy on the apparent Schmid factor distribution at the free surface of polycrystals is presented. Cubic elasticity is considered. Order II stresses (averaged on all grains with the same crystallographic orientation) as well as variations between averages computed on grains with the same crystallographic orientation but with different neighbour grains are computed. The Finite Element Method is used. Commonly studied metals presenting an increasing anisotropy degree are considered (aluminium, nickel, austenite, copper). Concerning order II stresses in strongly anisotropic metals, the apparent Schmid factor distribution is drifted towards small Schmid factor values (the maximum Schmid factor is equal to 0.43 instead of 0.5) and the slip activation order between characteristic orientations of the crystallographic standard triangle is modified. The computed square deviations of the stresses averaged on grains with the same crystallographic orientation but with different neighbour grains are a bit higher than the second order ones (inter-orientation scatter). Our numerical evaluations agree quantitatively with several observations and measures of the literature concerning stress and strain distribution in copper and austenite polycrystals submitted to low amplitude loadings. Hopefully, the given apparent Schmid factor distributions could help to better understand the observations of the plasticity mechanisms taking place at the free surface of polycrystals. To cite this article: M. Sauzay, C. R. Mecanique 334 (2006).  相似文献   

18.
This paper is devoted to a micromechanics-based simulation of the response of concrete to hydrostatic and oedometric compressions. Concrete is described as a composite made up of a cement matrix in which rigid inclusions are embedded. The focus is put on the role of the interface between matrix and inclusion which represent the interfacial transition zone (ITZ). A plastic behavior is considered for both the matrix and the interfaces. The effective response of the composite is derived from the modified secant method adapted to the situation of imperfect interfaces. To cite this article: T.H. Le et al., C. R. Mecanique 336 (2008).  相似文献   

19.
The phenomena of hydrodynamic breakup of liquid jets, drops, films, bridges, and filaments are reviewed for liquids with viscoelastic properties. The reasons for breakup are capillary instabilities, collisions with rigid obstacles, and other forms of dynamic action. The relationship between the properties of the liquids and the features of the breakup process is discussed.  相似文献   

20.
Flow stability analysis and excitation using pulsating jets   总被引:1,自引:0,他引:1  
Classical flow stability applied to transition from laminar to turbulent flow may also describe the behavior of vorticity fluctuations created by a pulsating jet placed along a solid boundary. A numerical laminar flow experiment involving a pulsating jet placed along the surface of a duct with flow separation downstream, resulted in eliminating most part of the separated flow region. Applying the same approach to a turbulent flow, it was possible to develop a turbulent stability flow formulation and apply successfully turbulent pulsating jet flow separation control. To cite this article: D. Skamnakis, K. Papailiou, C. R. Mecanique 333 (2005).  相似文献   

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