单向纤维增强复合材料中纤维断裂及其发展

纤维增强复合材料中某根纤维断裂后，断口作为裂纹向何处发展？它可以向纤维和基体的界面发展形成界面脱粘，也可向基体发展，造成基体开展，从而殃及邻近纤维。另外，一根纤维的断裂会在其邻近纤维中造成应力集中。本文采取轴对称边界元法对这些问题进行仔细研究。本文假定纤维在基体中成六角形分布，即每根纤维周围有六根纤维，均匀地分布在以该纤维为中心的圆周上。     

纤维／基体界面裂纹扩展断裂能

本文通过研究纤维／基体界面裂纹断裂能，分析了几种界面脱粘断裂功的理论表达式；着重研究了单纤维拔出试验中界面残余压应力及界面摩擦对界面裂纹能量释放率的重要性．     

正交复合材料层板断裂模型的研究

正交铺设复合材料层板裂纹自相似扩展时的断裂模型可看作为在正交各向异性材料中主裂纹前缘嵌入一个由多根分枝裂纹构成的损伤区。损伤区外部的应力场和位移场可按正交各向异性断裂力学公式来计算。本文研究了多根分枝裂纹和所引起的根部纤维应力松弛的规律,并建议了预测复合材料断裂韧性K_c值的方法,所得值与实验结果相符。     

各向异性编织CMC弯曲断裂失效模型

通过对缺口弯曲断裂试验的研究发现，编织CMC存在两种断裂失效模式：界面主导的和纤维束主导的失效模式．针对这两种模式建立了界面失效模型和纤维束断裂失效模型．界面失效模型用半经验方法处理弱界面和大编织角度的断裂强度问题；纤维束断裂失效模型采用解析方法处理较强界面和小角度的断裂强度问题，为含有缺口试件的弯曲强度预报打下了初步的理论基础．     

钨/铜复合材料纤维断裂瞬态行为的声发射源特征法

<正> 1 引言 纤维增强复合材料的断裂,一般包括三个过程:①基体与纤维界面的脱粘,②纤维断裂;③基体中的裂纹扩展。从复合材料承载能力的观点来看,纤维断裂最为重要,所以根据内应力在纤维中的重新分布对复合材料的破坏进行了某些分析。但这些研究局限于静态分析,而高强度脆性纤维的断裂实际上是一个动态过程,它伴随着有能量的突      

复合材料内由纤维断裂引起的应力集中

在研究复合材料的断裂和强度时,由纤维断裂引起的应力集中是必须首先知道的.在纤维断点附近的应力集中己有不少研究.本文着重研究当应力波沿纤维方向传播时,离纤维断点有一定距离处的动应力集中系数.     

断裂问题特征根的重根探讨

利用特征矩阵的秩与特征根所对应的子特征函数空间维数之间的关系。确定了反平面断裂问题和平面断裂问题的特征根可能出现的最大重根数．利用Reissner型板特征根与反平面和平面断裂问题特征根的关系确定其可能出现的最大重根数．得到了反平面断裂问题、平面断裂问题和Reissner板断裂问题可能出现的最大重根数分别为1,2,3．     

高温环境下纤维复合材料蠕变损伤的细观机理研究

首先利用复合材料纤维断裂单胞模型，编制蠕变损伤子程序，对单胞模型进行蠕变损伤分析。分析了纤维／基体弹性模量比对蠕变变形、蠕变损伤以及应力场的影响。从计算结果发现，蠕变损伤首先在纤维断裂尖端起始，然后沿着一定的角度向基体外围延伸，直至完全损伤，而且纤维／基体模量比对高温环境下的复合材料蠕变损伤产生很大的影响；纤维与基体的模量相差越大，复合材料越容易变形，抵抗蠕变变形的能力就越小，蠕变损伤越严重。经过对不同韧性的基体材料进行研究，发现基体韧性低的复合材料蠕变损伤明显高于高韧性基体复合材料，表明低韧性基体复合材料抵抗蠕变破坏的能力较低。     

炭纤维增强聚四氟乙烯复合材料在干摩擦和水润滑条件下的摩擦学行为对比研究

对比考察了炭纤维增强聚四氟乙烯(PTFE)复合材料在干摩擦和水润滑条件下的摩擦磨损性能，并探讨了其磨损机理。结果表明：在水润滑条件下，纤维增强PTFE复合材料的摩擦系数和磨损率均明显比干摩擦下的低，水起到了润滑和冷却作用；复合材料磨损表面可见明显的裸露纤维及纤维局部磨平，无明显微观裂纹，基体和纤维结合较好，磨损表面存在转移自偶件的铁，表现出犁削磨损特征；在干摩擦下，复合材料磨损表面存在大量的微观断裂裂纹，纤维发生断裂和破碎，表现出疲劳磨损特征。     

复合材料的裂纹动力学问题的模型

复合材料产生裂纹后，其纤维处形成“桥连”，这是一个不可避免的现象。由于桥连问题很复杂，在数学方法的处理上有很大困难，至今人们研究的大多是桥连的静力学问题，而对其动力学问题研究得很少。只有建立复合材料的桥连动力学模型，才能更好地研究复合材料的断裂动力学问题。为了便于分析复合材料的问题，将桥连处用载荷代替，当裂纹高速扩展时，其纤维也连续地断裂。通过复变函数论的方法，将所讨论的问题转化为Riemann-Hilbet问题。利用建立的动态模型和自相似方法，得到了正交异性体中扩展裂纹受运动的集中力Px/t及均布载荷作用下位移、应力和动态应力强度因子的解析解，并通过迭加原理，最终求得了该模型的解。     

A variational method for unidirectional fiber-reinforced composites with matrix creep

A variational method is developed for analyzing the matrix creep induced time-dependent change in fiber stress profiles in unidirectional composites. A functional of admissible profiles of fiber stress rate is presented by supposing a fiber broken in matrix as well as a fiber pulled out from matrix. The functional is shown to have the stationary function satisfying an incremental differential equation based on the shear lag assumption. Then, the stationary function is approximately determined by assuming bilinear profiles of fiber stress and a power law of matrix creep, leading to analytical solutions for the time-dependent change in fiber stress profiles. The solutions are verified on the basis of an energy balance equation and a finite difference computation. Moreover, it is shown that the solution for the fiber pull-out model agrees well with an experiment on a single carbon fiber/acrylic model composite if the initial slip at fiber/matrix interface is taken into account. In addition, the solution for the fiber breakage model is used for evaluating the characteristic time in long-term creep rupture of unidirectional composite.     

聚氨酯泡沫塑料动态剪切力学行为的研究

通过大型精密分段式Ｈｏｐｋｉｎｓｏｎ 扭杆实验装置对聚氨酯泡沫塑料进行了动态扭转实验,研究了聚氨酯泡沫塑料在剪切应力波加载下的力学行为,得到了这类材料的动态剪切应力 应变曲线和动态力学性能参数。此外,针对动态扭转破坏试件断口进行了扫描电镜分析,研究了泡沫塑料动态剪切破坏的机制。还给出了同准静态扭转实验结果的比较。     

Effect of fiber geometry on stress in fiber-reinforced composite materials

Eleven two-dimensional photoelastic models of fiber-reinforced composite-material configurations were designed for the purpose of investigating the effects of various fiber-end shapes, various fiber arrangements and broken fibers on the shear-stress distribution in an elastic matrix. Maximum shear stresses in the matrix in the vicinity of fiber discontinuities are presented. The peak stress resulting from a gradually tapered fiber was found to be slightly higher than that from a square-ended fiber, and a round-ended fiber produced a peak stress which was slightly lower than that from the square-ended fiber. Peak stresses resulting from two square-ended fibers butted closely together were considerably higher and decreased with increasing gap length between fiber ends. It made little difference whether the gap between the butted fiber ends was open, simulating a void resulting from a broken fiber, or filled with matrix material.Paper was presented at 1966 SESA Spring Meeting held in Detroit, Mich., on May 4–6.     

Three-dimensional continuum analysis for a unidirectional composite with a broken fiber

The three-dimensional problem of a periodic unidirectional composite with a penny-shaped crack traversing one of the fibers is analyzed by the continuum equations of elasticity. The solution of the crack problem is represented by a superposition of weighted unit normal displacement jump solutions, everyone of which forms a Green’s function. The Green’s functions for the unbounded periodic composite are obtained by the combined use of the representative cell method and the higher-order theory. The representative cell method, based on the triple discrete Fourier transform, allows the reduction of the problem of an infinite domain to a problem of a finite one in the transform space. This problem is solved by the higher-order theory according to which the transformed displacement vector is expressed by a second order expansion in terms of local coordinates, in conjunction with the equilibrium equations and the relevant boundary conditions. The actual elastic field is obtained by a numerical evaluation of the inverse transform. The accuracy of the suggested approach is verified by a comparison with the exact analytical solution for a penny-shaped crack embedded in a homogeneous medium. Results for a unidirectional composite with a broken fiber are given for various fiber volume fractions and fiber-to-matrix stiffness ratios. It is shown that for certain parameter combinations the use of the average stress in the fiber, as it is employed in the framework of the shear lag approach, for the prediction of composite’s strength, leads to an over estimation. To this end, the concept of “point stress concentration factor” is introduced to characterize the strength of the composite with a broken fiber. Several generalizations of the proposed approach are offered.     

聚氨酯泡沫塑料的强度与断裂韧性

针对3种密度的聚氨酯泡沫塑料进行了拉伸实验。通过无缺口试件确定了3种密度泡沫塑料的拉伸断裂强度,而利用有缺口试件确定了这些材料的拉伸断裂韧性。为了研究高密度泡沫塑料的拉伸断裂机制,还对破坏后试件进行了扫描电镜分析。此外,还简要讨论了泡沫塑料拉伸断裂力学性能的理论预测问题。     

Stress relaxation in broken fibers in unidirectional composites: modeling and application to creep rupture analysis

This paper describes a model of stress relaxation in broken fibers in unidirectional metal matrix composites reinforced with long brittle fibers. A cylindrical cell with a broken fiber embedded in a power law creeping matrix is employed, and the broken fiber is assumed to have a bilinear distribution of axial stress. Then, on the basis of energy balance in the cell under constant overall strain, a relaxation equation of interfacial shear stress acting on stress recovery segments is derived in a simple form. The relaxation equation is approximated rationally and integrated to obtain an analytical solution, which is shown to agree fairly well with the numerical analysis of Du and McMeeking. (Du, Z.-Z., McMeeking, R.M., 1995. Creep models for metal matrix composites with long brittle fibres. J. Mech. Phys. Solids 43, 701–726.) Moreover, the relaxation equation is combined with Curtin's model (Curtin, W.A., 1991. Theory of mechanical properties of ceramic-matrix composites. J. Am. Ceram. Soc. 74, 2837–2845.), so that rupture time in long term creep is evaluated analytically and explicitly on the assumption of global load sharing. It is shown that the resulting relation represents well the dependence of creep rupture time on applied stress observed experimentally on a unidirectional metal matrix composite.     

Intensity of singular stress at the fiber end in a hexagonal array of fibers

To evaluate the mechanical strength of fiber-reinforced composites it is necessary to consider singular stresses at the end of fibers because they cause crack initiation, propagation, and final failure. The singular stress field is controlled by generalized stress intensity factor (GSIF) defined at the fiber end. In this study, periodic and zigzag arrays of cylindrical inclusions under longitudinal tension are considered in comparison with the results for a single fiber. The unit cell region is approximated as an axi-symmetric cell; then, the body force method is applied, which requires the stress and displacement fields due to ring forces in infinite bodies having the same elastic constants as those of the matrix and inclusions. The given problem is solved on the superposition of two auxiliary problems under different boundary conditions. To obtain the GSIF accurately, the unknown body force densities are expressed as piecewise smooth functions using fundamental densities and power series. Here, the fundamental densities are chosen to represent the symmetric stress singularity, and the skew-symmetric stress singularity. The GSIFs are systematically calculated with varying the elastic modulus ratio and spacing of fibers. The effects of volume fraction and spacing of fibers are discussed in fiber-reinforced plastics.     

Uncertainties of unidirectional composite strength under tensile loading and variation of environmental condition

A probabilistic strength model is developed for unidirectional composites with fibers in hexagonal arrays. The model assumes that, a central core of broken fibers surrounded by unbroken fibers which are subjected to unidirectional tensile loading. The proposed approach consists in using a modified shear lag model to calculate the ineffective lengths and stress concentrations around fiber breaks. The main feature in the model lies in incorporating the variation of composite properties due to temperature and moisture, in order to predict degradation of fibers and matrix characteristics. The strength degradation is often seen as a result of changes in ineffective lengths at fiber breaks, leading to stress concentrations in intact neighboring fibers. As fiber breaks are intrinsically random, the variability of input data allows us to describe the probabilistic model by using the Monte-Carlo method. The sensitivities of the mechanical response are evaluated regarding the uncertainties in design variables such as Young’s modulus of fibers and matrix, fiber reference strength, shear yield stress, fiber volume fraction and shear parameter defining the shear stress in the inelastic region.     

纤维段裂试验的界面端应力奇异性研究

纤维段裂试验是测定纤维复合材料界面剪切强度的细观实验方法之一，其试验结果与其他三种细观试验方法(纤维拔出、纤维压人和微珠脱粘)测得的结果各不相符，相差较大。针对该问题，仔细研究了纤维段裂试验过程，可发现如下两个问题，首先是试件中纤维断裂造成的界面端应力奇异性问题；其次是纤维断成临界长度时界面是否脱粘的问题。针对界面端应力奇异性问题，本文建立了界面端轴对称分析模型，运用渐近展开法，推导出求解界面端特征值的特征方程，并由此得到应力奇异性指数随Dundurs常数的变化规律；采用文献[5]所用试件的纤维／基体性能数据，计算出了界面端的应力奇异性指数，并与文献[7]得到的其他三种试验的界面端应力奇异性指数进行比较，发现纤维段裂试件也存在界面端应力奇异性，而且应力奇异性最强，也说明了与其他三种试验结果不具可比性。本文还对纤维断成临界长度时界面是否脱粘的问题，进行了讨论。