ѧÊõÔ¤¸æ Ê×Ò³  >  ѧÊõ¿ÆÑÐ  >  ѧÊõÔ¤¸æ  >  ÕýÎÄ

¡°Á½Ð£Ãûʦ½²Ìá±Ñ§ÊõÔ¤¸æ263¡ªMixed Finite Element Methods of Elasticity Problems
×÷Õߣº     ÈÕÆÚ£º2018-11-14     À´Ô´£º    

½²×ùÖ÷Ì⣺Mixed Finite Element Methods of Elasticity Problems

ר¼ÒÐÕÃû£ººú¿¡

¹¤×÷µ¥Î»£º±±¾©´óѧ

½²×ùʱ¼ä£º2018Äê11ÔÂ16ÈÕ17ʱ0·Ö

½²×ùµØµã£ºÊýѧѧԺ340

Ö÷°ìµ¥Î»£º×ðÁú¿­Ê±¹ÙÍøÊýѧÓëÐÅÏ¢¿ÆÑ§Ñ§Ôº

ÄÚÈÝÕªÒª£º

The problems that are most frequently solved in scientific and engineering computing may probably be the elasticity equations. The finite element method (FEM) was invented in analyzing the stress of the elastic structures in the 1950s. The mixed FEM within the Hellinger-Reissner (H-R) principle for elasticity yields a direct stress approximation since it takes both the stress and displacement as an independent variable. The mixed FEM can be free of locking for nearly incompressible materials, and be applied to plastic materials, and approximate both the equilibrium and traction boundary conditions more accurate. However, the symmetry of the stress plus the stability conditions make the design of the mixed FEM for elasticity surprisingly hard. In fact, ``Four decades of searching for mixed finite elements for elasticity beginning in the 1960s did not yield any stable elements with polynomial shape functions" [D. N. Arnold, Proceedings of the ICM, Vol. I : Plenary Lectures and Ceremonies (2002)]. Since the 1960s, many mathematicians have worked on this problem but compromised to weakly symmetric elements, or composite elements. In 2002, using the elasticity complexes, Arnold and Winther designed the first family of symmetric mixed elements with polynomial shape functions on triangular grids in 2D.

The talk presents a new framework to design and analyze the mixed FEM of elasticity problems, which yields optimal symmetric mixed FEMs. In addition, those elements are very easy to implement since their basis functions, based on those of the scalar Lagrange elements, can been explicitly written down by hand. The main ingredients of this framework are a structure of the discrete stress space on both simplicial and product grids, two basic algebraic results, and a two-step stability analysis method.

Ö÷½²È˽éÉÜ£º

ºú¿¡£¬ ±±¾©´óѧÊýѧ¿ÆÑ§Ñ§Ôº½ÌÊÚ¡¢µ³Î¯Êé¼Ç£¬ ¹ú¼Ò½Ü³öÇàÄê»ù½ð»ñµÃÕß¡£ Ö÷Òª´ÓÊ·DZê×¼ÓÐÏÞÔª·½·¨£¬ÌرðÊǵ¯ÐÔÁ¦Ñ§ÎÊÌâ¼°Ïà¹ØÎÊÌâµÄ·Ç±ê×¼ÓÐÏÞÔª·½·¨µÄ¹¹Ôì¡¢ÊýÖµ·ÖÎö¼°×ÔÊÊÓ¦ÓÐÏÞÔª·½·¨µÈ·½ÃæµÄÑо¿¡£·¢±íÏà¹ØÁìÓòµÄÂÛÎÄ60ÓàÆª£¬Ôø»ñÖйú¼ÆËãÊýѧѧ»áµÄ¡°Ê×½ìÇàÄ괴н±¡±£¬È«¹ú°ÙƪÓÅÐ㲩ʿѧλÂÛÎĺ͵¹úºé±¤Ñо¿½±Ñ§½ðµÈÈÙÓþ¡£ ÏÖÈÎÈý¸ö¹ú¼ÊÆÚ¿¯µÄ±àίºÍ±±¾©¼ÆËãÊýѧѧ»áÀíʳ¤¡£

°Ù¶ÈһϠËÑË÷ ×ðÁú¿­Ê± - ÈËÉú¾ÍÊDz«!