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内聚力界面单元在胶接接头分层仿真中的应用 总被引:1,自引:0,他引:1
分层是胶接接头的主要破坏形式,而分层主要发生在胶层与被粘物的界面层上,因此,对胶接接头界面层的力学行为的分析是很有必要的.由于界面层厚度太小,用常规的有限元法或边界元法很难对其进行仿真,更加无法仿真胶接接头的分层损伤过程.针对上述情况,为提高接头结构承载力,采用零厚度的内聚力界面单元来仿真界面层,克服无法仿真界面层的困难,对胶接接头的分层损伤过程进行仿真,并与试验结果进行对比,验证方法的有效性.通过仿真分析结果与试验结果对比可知,仿真分析结果与试验结果吻合较好.因此,运用内聚界面单元仿真界面层方法是有效的,并为复杂胶接接头承载能力分析提供有力的依据. 相似文献
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基于代表性体积单元和内聚力模型,使用内聚力单元和扩展有限元方法分别模拟界面损伤和基体损伤,通过ABAQUS二次开发建立了纤维增强复合材料细观力学模型。以受横向拉伸的碳纤维/树脂代表性体积单元为研究对象,分析对比了不同强度下仅考虑界面损伤时复合材料的力学特性和同时考虑界面、基体损伤时的力学特性。结果表明纤维对基体的增强效果随界面强度提高;扩展有限元方法能在不依赖网格数量的条件下准确描述基体中多条裂纹的萌生及扩展过程,并且捕捉到基体裂纹引起的界面损伤;仅考虑界面损伤时的代表性体积单元平均应力-位移曲线后期呈上升趋势,而同时考虑界面和基体损伤的平均应力-位移曲线后期呈下降趋势。 相似文献
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为准确分析型钢混凝土柱的抗火灾行为,采用Abaqus软件对型钢混凝土十字形柱进行顺序热力耦合分析,将十字形柱的截面温度分布、温度-时间关系、火灾后的破坏模式以及载荷-位移关系的模拟结果与试验结果进行对比,验证有限元模型的有效性。讨论十字形柱模型的参数敏感性,选择最优混凝土材料属性、建模单元和材料的热膨胀系数,为型钢混凝土组合结构模拟提供更精确的参考依据。 相似文献
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扩展的多尺度有限元法基本原理 总被引:3,自引:0,他引:3
阐述一种适用于非均质材料力学性能分析的扩展的多尺度有限元法(Extended Multiscale Finite Element Method,EMsFEM)的基本原理.该方法的基本思想是利用数值方法构造能反映胞体单元内部材料非均质影响的多尺度基函数,在此基础上求得粗网格层次的等效单元刚度阵,从而在粗网格尺度上对原问题进行求解,很大程度地减少计算量.以该方法进行的具有周期和随机微观结构的材料计算示例,通过与传统有限元法的结果比较,说明这一方法的有效性.EMsFEM的优势在于,能容易地进行降尺度计算,可较准确地求得单元内部的微观应力应变信息,在非均质材料强度和非线性分析中有很大的应用潜力. 相似文献
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为了研究岩石表面变形破坏过程的变化特征,设计了一个可视化应用程序.该应用程序以岩石常规力学性质试验视频作为研究对象,包括静态图像处理界面和视频图像处理界面.静态图像处理界面由图像类型转换、图像边缘检测、图像形态学处理、图像滤波处理4个模块组成.视频处理界面则提供试验视频帧数、历时、帧图像大小和维数等基本信息.通过在可视化界面上进行所需参数设置实现了单帧图像特征纹理参数计算和岩石试样表面位移场的计算.本文还以两个示例说明了使用该应用程序进行岩石材料变形破坏过程分析的方法.本文成果对分析岩石材料变形特点和破坏机制具有一定的参考价值. 相似文献
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基于非局部近场动力学(Peridynamics,PD)理论,对含预置裂纹的混凝土巴西圆盘劈裂破坏问题进行建模分析.将结构离散为包含混凝土材料信息的粒子,引入动态松弛、分级加载和失衡力守恒等粒子系统数值算法,构建可以自然模拟脆性裂纹扩展的PD算法体系.对含不同角度单预置中心裂纹巴西圆盘的裂纹扩展过程进行数值模拟,所得结果与试验结果吻合较好,验证所提出的模型和算法正确.进一步采用该方法模拟双预置裂纹巴西圆盘劈裂破坏过程中的裂纹扩展、交汇、贯通过程,通过将所得模拟结果与试验结果进行比较分析,探究该方法处理多裂纹扩展问题的可行性. 相似文献
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采用相对描述方式建立了Sandia国家实验室结构连接件与界面研究中提出的对称连接梁Benchmark问题的对称和反对称动力学模型,解析分析了系统的模态特性.解析模型中连接段采用挠性根部法模拟其变形势能,根部挠性参数则根据试验结果识别.并采用虚拟材料法模拟连接段进行了有限元分析.两种方法均获得了该Benchmark模型与其模态试验结果一致的动态特性. 相似文献
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An open source program to generate zero-thickness cohesive interface elements in existing finite element discretizations is presented. This contribution fills the gap in the literature that, to the best of the author’s knowledge, there is no such program exists. The program is useful in numerical modeling of material/structure failure using cohesive interface elements. The program is able to generate one/two dimensional, linear/quadratic cohesive elements (i) at all inter-element boundaries, (ii) at material interfaces and (iii) at grain boundaries in polycrystalline materials. Algorithms and utilization of the program is discussed. Several two dimensional and three dimensional fracture mechanics problems are given including debonding process of material interfaces, multiple delamination of composite structures, crack propagation in polycrystalline structures. 相似文献
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J.W. Foulk 《Computer Methods in Applied Mechanics and Engineering》2010,199(9-12):465-470
Stable crack propagation hinges on the driving force and the resistance. In the context of a cohesive approach to fracture, properly resolving the cohesive zone ensures that the resistance is in equilibrium with the driving force. Additional restrictions on the mesh size can stem from crack stability. For high strength, low toughness (brittle) materials, the requirements for stability can exceed those for cohesive zone resolution. Examples in 1-D and 2-D reveal that decrements in the mesh size transition the system from indefinite to positive definite. Moreover, small decreases in the mesh size beyond the transition provide substantial reductions in the condition number. We contrast a physical instability resulting from material properties, geometry, or boundary conditions from a numerical instability resulting from the mesh size and propose that the selected discretization should ensure that the cohesive zone is both resolved and stabilized. 相似文献
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M. Samimi J.A.W. van Dommelen M.G.D. Geers 《Computer Methods in Applied Mechanics and Engineering》2011,200(49-52):3540-3553
Discrete crack models with cohesive binding forces in the fracture process zone have been widely used to address failure in quasi-brittle materials and interfaces. However, the numerical concerns and limitations stemming from the application of interface cohesive zone models in a quasi-static finite element framework increase considerably as the relative size of the process zone decreases. An excessively fine mesh is required in the process zone to accurately resolve the distribution of tractions in a relatively small moving zone. With a moderate mesh size, inefficient path-following techniques have to be employed to trace the local discretization-induced snap-backs. In order to increase the applicability of cohesive zone models by reducing their numerical deficiencies, a self-adaptive finite element framework is proposed, based on a hierarchical enrichment of the standard elements. With this approach, the planar mixed-mode crack growth in a general three-dimensional continuum, discretized by a coarse mesh, can be modeled while the set of equations of the non-linear system is solved by a standard Newton–Raphson iterative procedure. This hierarchical scheme was found to be most effective in reducing the oscillatory behavior of the global response. 相似文献
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In this paper, a mesoscale model of concrete is presented, which considers particles, matrix material and the interfacial
transition zone (ITZ) as separate constituents. Particles are represented as ellipsoides, generated according to a prescribed
grading curve and placed randomly into the specimen. Algorithms are proposed to generate realistic particle configurations
efficiently. The nonlinear behavior is simulated with a cohesive interface model for the ITZ. For the matrix material, different
damage/plasticity models are investigated. The simulation of localization requires to regularize the solution, which is performed
by using integral type nonlocal models with strain or displacement averaging. Due to the complexity of a mesoscale model for
a realistic structure, a multiscale method to couple the homogeneous macroscale with the heterogeneous mesoscale model in
a concurrent embedded approach is proposed. This allows an adaptive transition from a full macroscale model to a multiscale
model, where only the relevant parts are resolved on a finer scale. Special emphasis is placed on the investigation of different
coupling schemes between the different scales, such as the mortar method and the arlequin method, and a discussion of their
advantages and disadvantages within the current context. The applicability of the proposed methodology is illustrated for
a variety of examples in tension and compression. 相似文献
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G. Becker C. Geuzaine L. Noels 《Computer Methods in Applied Mechanics and Engineering》2011,200(45-46):3223-3241
In order to model fracture, the cohesive zone method can be coupled in a very efficient way with the finite element method. Nevertheless, there are some drawbacks with the classical insertion of cohesive elements. It is well known that, on one the hand, if these elements are present before fracture there is a modification of the structure stiffness, and that, on the other hand, their insertion during the simulation requires very complex implementation, especially with parallel codes. These drawbacks can be avoided by combining the cohesive method with the use of a discontinuous Galerkin formulation. In such a formulation, all the elements are discontinuous and the continuity is weakly ensured in a stable and consistent way by inserting extra terms on the boundary of elements. The recourse to interface elements allows to substitute them by cohesive elements at the onset of fracture.The purpose of this paper is to develop this formulation for Kirchhoff–Love plates and shells. It is achieved by the establishment of a full DG formulation of shell combined with a cohesive model, which is adapted to the special thickness discretization of the shell formulation. In fact, this cohesive model is applied on resulting reduced stresses which are the basis of thin structures formulations. Finally, numerical examples demonstrate the efficiency of the method. 相似文献
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We present a simple set of data structures, and a collection of methods for constructing and updating the structures, designed
to support the use of cohesive elements in simulations of fracture and fragmentation. Initially, all interior faces in the
triangulation are perfectly coherent, i.e. conforming in the usual finite element sense. Cohesive elements are inserted adaptively
at interior faces when the effective traction acting on those faces reaches the cohesive strength of the material. The insertion
of cohesive elements changes the geometry of the boundary and, frequently, the topology of the model as well. The data structures
and methods presented here are straightforward to implement, and enable the efficient tracking of complex fracture and fragmentation
processes. The efficiency and versatility of the approach is demonstrated with the aid of two examples of application to dynamic
fracture. 相似文献
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L. P. Yeo S. C. Joshi Y. C. Lam Mary B. Chan-Park D. E. Hardt 《Microsystem Technologies》2009,15(4):581-593
Ultraviolet (UV) embossing, involving molding against micro-structured molds, is a quick and efficient method to mass produce
high aspect ratio micro-features. A crucial challenge to the repeatability and large-scale application of this technique is
successful demolding, which escalates in difficulty with increasing aspect ratio, due to increased polymer-mold mechanical
interlocking. Some of the key factors affecting UV embossing include the crosslinked polymer shrinkage and material properties,
interfacial strength between polymer to mold and the demolding method. This paper presents a new method to simulate the demolding
of UV cured polymer from a nickel mold. Hyperelastic material model and rate-independent cohesive zone modeling were employed
in the numerical simulation; linear elastic polymer response, although relatively easy to apply, was not adequate. Progressive
shrinkage was implemented, leading to delamination of the polymer-mold interface. The subsequent peeling of the cured polymer
from the mold was modeled with increasing prescribed displacement. The optimal shrinkage degree was found to increase from 0.92 to 1.9% with increasing mold aspect ratio (aspect ratio is defined
as height to width ratio) from 5 to 10. 相似文献