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1.
提出了一种以栅格法为基本方法,基于几何特征和物理场量双重自适应的六面体网格再生成方法。首先,依据旧网格的表面曲率和几何特征,采用基于栅格法的几何自适应网格再生成方法,生成密度受控的基础网格;然后,将旧网格的物理场量传递到基础网格中;最后,采用有限元误差估计方法对新网格单元的计算误差进行估计,对误差较大的单元进行加密,减...  相似文献   

2.
提出多结点六面体单元的结点形函数构建方法,解决了数字化分析时两个多尺度有限元网格在接触界面由于单元结点不匹配而导致的结点属性不能连续传递问题.首先将全局坐标下的六面体单元及其表面上多结点通过等参逆变换转成局部坐标下的规则六面体单元及其表面上多结点;在规则单元中,以每个结点为基点,分别沿三个正交的局部坐标方向在单元内寻找...  相似文献   

3.
介绍一种基于Delaunay算法的四面体自适应网格的自动划分方法。该方法用单元尺度场控制生成网格的疏密分布,在不满足尺度场要求的单元面形心处插入新节点,同时计算新节点单元尺寸参数,实现三维实体的Delaunay四面体自动划分。此方法具有几个特点:一是表面网格与体内网格同步划分,无需区分两者;二是结点与单元同时生成;三是生成网格自适应性好,疏密分布任意。另外,还介绍了三维网格划分中两个相关算法:一个是约束面恢复算法,该算法基于约束面不允许有单元边与之相交的性质而提出的;另一个是将二维射线法推广至三维空间,判断一个点是否在一多面体内,实现了凹多面体的划分。最后通过算例对单元质量进行了评价。本文所述方法是一种有效的四面体自适应单元生成算法。  相似文献   

4.
针对两零件的异构网格单元结点在接触界面不能相互匹配导致结点属性不能连续过渡和传递的问题,提出非匹配结点的有限单元等参插值方法,通过构建非匹配结点的形函数和修正原结点的形函数,将结点属性值的影响范围限制在可控的局部区域,从而实现两异构网格结点属性在接触界面的连续过渡和传递。通过两个异构的四边形单元网格的结点属性在接触界面的过渡实例和啮合齿轮的接触分析应用,验证了该方法的正确性和有效性。  相似文献   

5.
为描述钢筋混凝土柱的破坏过程,分别建立了由三维实体单元和三维杆单元构成的精细化模型以及结合纤维梁单元的纤维梁与实体单元耦合模型。耦合模型中,钢筋混凝土柱下段混凝土和钢筋分别用三维实体单元与三维杆单元建模,通过耦合连接实现精细单元与粗糙单元之间的变形协调。基于混凝土弹塑性本构关系,运用扩展有限元方法模拟钢筋混凝土柱的荷载-位移曲线以及开裂过程,并进行比较。数值模拟与试验结果的比较表明,模拟得到的裂缝位置以及荷载-位移曲线与试验结果吻合较好。扩展有限元具有无需重划网格、无需预设裂纹的优点,能有效地模拟筋混凝土柱的开裂过程。耦合模型具有计算效率高的优势,且能较好地模拟构件的破坏模式。  相似文献   

6.
剖分是进行有限元计算的前期工作,它主要是通过网格化,将实体划分成具有相同类型的单元。本文采用由外向内的部分思路,利用10节点四面体等参数单元,实现了对三维不对称实体的网格剖分。计算结果表明,使用本文的剖分算法进行后期的有限元计算是十分理想的。  相似文献   

7.
以映射法为基础并结合网格划分经验,提出了原理简单的六面体网格生成新办法.该方法根据物体轮廓选择初始网格,设定表面结点强制变形到目的曲面,经由有限元弹性计算确定内部节点的位置.在检查全体单元质量以后,调整畸形单元从而生成目的网格.通过为一个复杂的马头门模型构建全六面体网格,最后证明了本文所述方法的可行性.  相似文献   

8.
利用非线性有限元方法分析了轴向力作用下多平面TT节点的极限强度。在数值分析中,采用三维20结点固体单元模拟管道结构和焊缝形状,将结构有限元网格划分为不同区域,每个区域的网格独立产生,通过合并形成整个结构的有限元网格。通过控制位移增量法得到了加载过程中载荷和位移之间的关系曲线。使用ABAQUS软件分析了TT节点在支管端部承受轴向载荷的变形及与外部载荷之间的关系,得到了不同参数影响下的TT节点极限强度。  相似文献   

9.
三维有限元六面体网格几何自适应再生成方法   总被引:2,自引:1,他引:1  
基于几何自适应的六面体网再生成方法,提出了一种以栅格法为基本方法,对有限元网格再划分过程中的网格再划分标准、几何形状的获取以及新旧网格之间物理量的传递等关键问题进行了研究.重点介绍了基于几何自适应的六面体网格再生成算法,首先对旧网格实体模型进行识别,根据实体模型几何特征建立加密源点信息场;然后采用栅格法生成核心网格并对...  相似文献   

10.
一种人—机结合的二维有限元网格生成方法   总被引:1,自引:0,他引:1  
唐国安  王皓 《力学季刊》1992,13(4):76-81
本文提出了一种人一机结合的二维有限元网格生成方法,可将在CAD环境下绘制的矢量型网格图形自动地转换为有限元分析时所用的结点坐标和单元组信息。此方法能完全按人的意图生成网格形状,但比人工划分大大节省时间,而且对计算机硬件要求甚低,在任何PC机上都可应用、  相似文献   

11.
喻虹 《爆炸与冲击》2003,23(6):493-500
针对大变形流体动力学数值计算中经常需要应用的网格重构与物理量重映技术,提出了一种逻辑简单的质点积分守恒重映方法。将旧网格细分为众多有体积的质点,并将旧网格的物理量分配到各个质点,新网格各守恒量的积分直接由落在新网格内的所有质点的物理量累加。建立了收敛速度极快的计算格式,采用的控制体很好地解决了速度的重映计算问题。分析了此守恒重映方法的收敛性与守恒性,研究了积分控制体对速度计算的影响。  相似文献   

12.
This paper describes the use of overlapping grids for the calculation of flow around single and multipleparticle configurations at the micro scale. The basic equations for calculation are those for conservation of mass and momentum which are solved using a common Finite-Volume formulation. The hydrodynamic particle-particle and particle-wall interaction can be calculated by using an overlapping or Chimera grid scheme. With the grid structuring procedure it is possible to use simple and structured grids around the particles and the overall main grid geometry. The particle grids are lapped over the main grid such that they can move independently after each time step without remeshing the whole geometry. The paper gives results for the validation of the code developed for general test cases, for a rotating ellipsoid in simple shear flow, the flow around particles attached to a wall, the motion of a particle in the vicinity of a wall and some results for the flow through a packed bed configuration.  相似文献   

13.
断裂过程的有限元模拟   总被引:40,自引:0,他引:40  
讨论了材料断裂过程的有限元模拟技术。基于自适应有限元的一般原理,并针对多相材料的裂纹扩展的特点,提出了一种简化的高精度和高效率有限元网格的动态重新划分策略。裂纹被假设沿着单元之间的路径连续扩展,利用节点力释放技术生成新的裂纹自由表面,发展了一种可随裂尖连续移动的网格动态加密和释放方法。这种方法已在各种裂纹问题中得以实现与应用。  相似文献   

14.
一种有效的广义特征值分析方法   总被引:1,自引:0,他引:1  
提出了一种适合于自适应有限元分析中求解广义特征值问题的多重网格方法.这种方法充分利用了初始网格下的结果,通过插值或最小二乘拟合技术来得到网格变化后的新的近似特征向量,然后由多重网格迭代过程实现对结构广义特征值问题的求解.在多重网格迭代的光滑步中,选择了收敛梯度法以提高其收敛率;在粗网格校正步中,则导出了一种近似求解特征向量误差的方程.这种方法将网格离散过程和数值求解过程很好地相结合,建立了一个网格细分后广义特征值问题的快速重分析方法,与传统有限元方法相比较,具有计算简便、计算量少等特点,可以作为结构动力问题自适应有限元分析的一种十分有效的工具.  相似文献   

15.
Problems associated with finite element simulation of the forming processes are characterized by large elastoplastic deformations, evolutive contact with friction, geometrical nonlinearities inducing a severe distortion of the computational mesh of the domain. In this case, frequent remeshing of the deformed domain during computation are necessary to obtain an accurate solution and complete the computation until the termination of the numerical simulation process. This Note presents a new adaptive remeshing method of thin sheets for numerical simulation of metal forming processes. The proposed method is based on geometrical criteria and does not use the geometry of the forming tools. It is integrated in a computational environment using the ABAQUS solver. Numerical examples are given to show the efficiency of our approach. To cite this article: L. Moreau et al., C. R. Mecanique 333 (2005).  相似文献   

16.
A method for generating irregular triangular computational grids in two-dimensional multiply connected domains is described. A set of points around each body is defined using a simple grid generation technique appropriate to the geometry of each body. The Voronoi regions associated with the resulting global point distribution are constructed from which the Delaunay triangulation of the set of points is thus obtained. The definition of Voronoi regions ensures that the triangulation produces triangles of reasonable aspect ratios given a grid point distribution. The approach readily accommodates local clustering of grid points to facilitate variable resolution of the domain. The technique is generally applicable and has been used with success in computing triangular grids in multiply connected planar domains. The suitability of such grids for flow calculations is demonstrated using a finite element method for solution of the inviscid transonic flow over two- dimensional high-lift aerofoil configurations.  相似文献   

17.
A new method for generating finite element grids in two and three dimensions is developed. The method is based on a new search tree structure. The search tree is built upon triangles in two dimensions and tetrahedra in three dimensions. The density of elements can be varied throughout the computational domain. Efficient search algorithms for finding points in space and for finding the boundary of the domain have been developed. The speed of the grid algorithm will permit adaptive gridding during computation. The grid algorithm is generally applicable to both hydrodynamic as well as aerodynamic finite element computations. The technique has been used with success for gridding the North Sea-Skagerrak area.  相似文献   

18.
A Galerkin finite element method and two finite difference techniques of the control volume variety have been used to study magnetohydrodynamic channel flows as a function of the Reynolds number, interaction parameter, electrode length and wall conductivity. The finite element and finite difference formulations use unequally spaced grids to accurately resolve the flow field near the channel wall and electrode edges where steep flow gradients are expected. It is shown that the axial velocity profiles are distorted into M-shapes by the applied electromagnetic field and that the distortion increases as the Reynolds number, interaction parameter and electrode length are increased. It is also shown that the finite element method predicts larger electromagnetic pinch effects at the electrode entrance and exit and larger pressure rises along the electrodes than the primitive-variable and streamfunction–vorticity finite difference formulations. However, the primitive-variable formulation predicts steeper axial velocity gradients at the channel walls and lower axial velocities at the channel centreline than the streamfunction–vorticity finite difference and the finite element methods. The differences between the results of the finite difference and finite element methods are attributed to the different grids used in the calculations and to the methods used to evaluate the pressure field. In particular, the computation of the velocity field from the streamfunction–vorticity formulation introduces computational noise, which is somewhat smoothed out when the pressure field is calculated by integrating the Navier–Stokes equations. It is also shown that the wall electric potential increases as the wall conductivity increases and that, at sufficiently high interaction parameters, recirculation zones may be created at the channel centreline, whereas the flow near the wall may show jet-like characteristics.  相似文献   

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