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History of the Finite Element Method - Mathematics Meets Mechanics - Part I: Engineering Developments

机译:有限元方法的历史 - 数学符合力学 - 第一部分:工程发展

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The birth of variational calculus and the principle of virtual work goes back to the 17th and 18th century, and the first draft of a discrete variational method with "elementwise" triangular shape functions was given by Leibniz (1697). First analytical studies were made by Schellbach (1851) and then, already with numerical results, by Rayleigh (1877). The mathematician Ritz (1909) marks the first discrete (direct) variational method for the linear elastic Kirchhoff plate, and the engineer Galerkin (1915) published his seminal article on FEM for linear elastic continua, postulating the orthogonality of the residua of equilibrium with respect to the test functions, but both, Ritz and Galerkin, used test and trial functions within the whole domain as supports. Courant (1943) was the first to introduce triangular and rectangular "finite elements" for the 2D-St.-Venant torsion problem of a prismatic bar (Poisson equ.), and Clough and his team (1956) published the first modern 2D-FEM for arrowed aircraft wings. Also Wilson, Melosh and Taylor with their important schools, e.g. Bathe and Simo, promoted in Berkeley the new discipline of "Computational Mechanics". Argyris (since 1959 in Stuttgart) and Zienkiewicz (since 1965 in Swansea), together with Irons e.g., developed primal FEM in a systematic way: hierarchical classes of FEs with different topologies and ansatz techniques for solid and fluid mechanics. Mixed finite elements, advocated for non-robust problems, are usually based on dual mixed variational functionals (yielding saddle point problems) by Hellinger (1914), Prange (1916) and Reissner (1950). Important elements came, e.g., from Cruceix, Raviart (1973), Raviart, Thomas (1977) and Brezzi, Douglas, Marini (1987). For numerical stability of saddle point problems, the Brezzi-Babuska global (infsup) stability conditions have to be fulfilled. Rather new extensions and variants of FEM are XFEM by Belytschko (1996) and SFM (Singular Function Method) by Fix, Strang (1973) and Grisvard (1992), as well as Isogeometric Analysis by Hughes (2005). This chapter and also chapter 23 are restricted to linear elastic solid and structural mechanics. The topics are designed not only in a descriptive way with verbal comments on the origins, main features and the importance of publications on FEM, but moreover, essential steps of continuous and discrete variational theory, finite element algorithms and error estimators as a basis for adaptivity are communicated as concentrated as possible. This seems to be advantageous for conceiving the subjects.
机译:变分法和虚功原理的诞生可以追溯到17世纪和18世纪,并以“按元素”三角形状功能的离散变分法的初稿是由莱布尼茨(1697)给出。首先分析研究由Schellbach(1851年)以后,已经与数值结果,通过瑞利(1877年)提出和。数学家里兹(1909)标记的第一离散的(直接)用于将线状弹性基尔霍夫板变分法,并发表了他关于FEM开创性文章线状弹性连续体的工程师的Galerkin(1915),postulating平衡相对于所述残渣的正交到测试功能,但两者,里兹和辽金,所使用的全域作为载体内测试和试功能。新闻报(1943年)是第一个引进的三角形和长方形的“有限元”的棱柱杆的2D-圣文南扭转问题(泊松当量),和克拉夫和他的团队(1956年)出版了第一本现代2D-有限元箭头飞机机翼。此外威尔逊,Melosh和泰勒与他们的重要流派,例如洗澡和Simo,伯克利促进“计算力学”的新学科。阿吉里斯(因为在Stuttgart 1959)和对Zienkiewicz(因为在斯旺西1965),与例如电熨斗一起,开发原始FEM以系统的方式:具有不同拓扑结构的FE和拟设技术的分层类固体和流体力学。混合有限元素,主张非健壮的问题,通常通过海林格(1914),普兰奇(1916)与Reissner(1950)基于双混合变函(产生鞍点的问题)。重要内容来了,例如,从Cruceix,Raviart(1973年),Raviart,托马斯(1977年)和Brezzi,道格拉斯,马里尼(1987)。对于鞍点问题的数值稳定,Brezzi-的Babuska全球(infsup)稳定的条件必须满足。而是新的扩展和有限元的变体XFEM通过BELYTSCHKO(1996年)和SFM(奇异函数法)的修复,斯特朗(1973)和Grisvard(1992年),以及Isogeometric分析休斯(2005)。本章并且还章23被限制为线性的弹性固体和结构力学。该主题设计不仅在与起源口头意见,主要特点和有限元法出版物的重要性,但此外,连续和离散变分理论的基本步骤,有限元的算法和误差估计为适应性基础的描述方式尽可能浓缩连通。这似乎是为构思主题是有利的。

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    《GAMM Annual Meeting》|2014年||共44页
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    Erwin Stein;

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  • 入库时间 2022-08-21 02:55:39

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