• CN:11-2187/TH
  • ISSN:0577-6686

›› 1979, Vol. 15 ›› Issue (2): 1-23.

• 论文 •    下一篇

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弹性理论中广义变分原理的研究及其在有限元计算中的应用

钱伟长   

  1. 清华大学
  • 发布日期:1979-03-01

Studies on Generalized Variational Principles in Elasticity and their Applications in Finite Element Calculations

Chien Weichang   

  1. Tsing Hua University
  • Published:1979-03-01

摘要: 本文的目的在于说明怎样系统地建立各种广义变分原理,怎样合理地使用各种广义变分原理来改进有限元计算的成效。为了易于说明问题,本文只局限于弹性理论的各种广义变分原理,但其推广并不困难。本文指出,广义变分原理的泛函,可以系统地采用拉格朗日乘子法,把一般有条件的变分原理化为无条件的变分原理来唯一地决定的。拉格朗日所代表的物理量,可以通过变分求极值或驻值的过程求得,从而消除了在建立广义变分原理的泛函时,人们经常陷入的象猜谜一样的困境。本文也指出:我们同样可以用拉格朗日乘子法,把一般有多个条件的变分原理,化为条件个数较少的变分原理。我们称变分条件减少了的变分原理为各级不完全的广义变分原理。凡是全部变分条件都消除了的变分原理,称为完全的广义变分原理,或简称广义变分原理;实际上是完全无条件的变分原理。本文建立了弹性小位移变形理论中的各级不完全的广义位能原理和各级不完全的广义余能原理,包括从最小位能原理和最小余能原理分别导出的最完全的广义变分原理,且并证明了这两个弹性力学广义变分原理的泛函是等同的。在这些广义变分原理中,包括了HELLINGER REISSNER(1950)[1],[2],胡海昌-鹫津久一郎[3],[4]的广义变分原理。本文也建立了弹性大移位变形中的位能原理和余能原理,并建立了有关位能余能的各级不完全的广义变分原理,包括从大位移变形的最小余能原理分别导出的弹性力学广义变分原理,并且也证明了大位移变形情况下,这两个弹性力学的广义变分原理也是同等的。本文除了列举广义变分原理在有限元法上的众所周知的应用外,还补充三个比较重要的应用范围。

Abstract: The purpose of this paper is to give a systematic way of deriving various generalized variational principles in elasticity, and also to give some applications of these principles for improving the finite element techniques. It is, however, easy to apply these methods for solving problems in other fields. In the first, it is indicated that the functionals of these generalized variational principles can be obtained systematically by means of Lagrange multiplier method. The physical meaning of these multipliers can be determined uniquely through the variation processes. In this way, it is possible to eliminate the difficulty of finding the functionals in generalized principles. In the second place, through Lagrange multiplier method, it is possible to establish various derived variational principles with fewer conditions of variation than those of the original variational principle. These derived variational principles with fewer conditions of variation may be called the incomplete generalized variational principles, on the other hand, we may call the derived variational principles without any conditions of variation the complete generalized variational principles, or briefly the generalized variational principles. It is possible to establish various generalized variational principles, either completely or incompletely, for small displacement theory of elasticity, including two well-known generalized variarional principles derived from the principle of minimum potential energy, and from the principle of minimum complementary energy. The equivalence of these two generalized variational principles is proved. These generalized principles include also Hellinger (1914) [1]-Reissne (1950)[2] principle and H. C. Hu-Wushizu (1955) [3][4] principle. In is also possible to establish principles of potential energy and complementary energy in finite displacement theory of elasticity, and various related incomplete generalized variational principles. The equivalence of these generalized variational principles derived from minimum potential energy and from minimum complementary energy has also been proved in the finite displacement theory. In this paper, the well-known applications of generalized variational principles to finite element method are discussed. Three more ways of applications are also given.