Variational implementation of immersed finite element methods

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• 作者：Luca Heltai^a ; ^{luca.heltai@sissa.it} ; Francesco Costanzo^b ; ^{costanzo@engr.psu.edu}
• 关键词：Fluid structure interaction ; Immersed boundary methods ; Immersed finite element method ; Finite element immersed boundary method
• 刊名：Computer Methods in Applied Mechanics and Engineering
• 出版年：2012
• 期刊代码：27_00457825
• 类别：cp
• 出版时间：1 July, 2012
• 卷：229-232
• 期：Complete
• 页码：110-127
• 文件大小：1183 K

摘要

Dirac-未 distributions are often crucial components of the solid-fluid coupling operators in immersed solution methods for fluid-structure interaction (FSI) problems. This is certainly so for methods like the immersed boundary method (IBM) or the immersed finite element method (IFEM), where Dirac-未 distributions are approximated via smooth functions. By contrast, a truly variational formulation of immersed methods does not require the use of Dirac-未 distributions, either formally or practically. This has been shown in the finite element immersed boundary method (FEIBM), where the variational structure of the problem is exploited to avoid Dirac-未 distributions at both the continuous and the discrete level.

In this paper, we generalize the FEIBM to the case where an incompressible Newtonian fluid interacts with a general hyperelastic solid. Specifically, we allow (i) the mass density to be different in the solid and the fluid, (ii) the solid to be either viscoelastic of differential type or purely elastic, and (iii) the solid to be either compressible or incompressible. At the continuous level, our variational formulation combines the natural stability estimates of the fluid and elasticity problems. In immersed methods, such stability estimates do not transfer to the discrete level automatically due to the non-matching nature of the finite dimensional spaces involved in the discretization. After presenting our general mathematical framework for the solution of FSI problems, we focus in detail on the construction of natural interpolation operators between the fluid and the solid discrete spaces, which guarantee semi-discrete stability estimates and strong consistency of our spatial discretization.