In this paper an application of the additive multilevel iteration method to parallel solving of large-scale linear elasticity problems is considered. The results are derived in the framework of the hierarchical basis finite element discretization defined on a tensor product xy β Tz of one-dimension
On a robust and scalable linear elasticity solver based on a saddle point formulation
β Scribed by Owe Axelsson; Alexander Padiy
- Publisher
- John Wiley and Sons
- Year
- 1999
- Tongue
- English
- Weight
- 461 KB
- Volume
- 44
- Category
- Article
- ISSN
- 0029-5981
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β¦ Synopsis
This paper presents a newly developed iterative algorithm for solving problems of linear isotropic elasticity discretized by means of mixed ΓΏnite elements. It continues work started in References 1-5. The proposed method uses a pressure Schur complement approach to solve a saddle-point system arising in the mixed formulation. As an inner solver for the displacement ΓΏeld variables it uses an extension to the robust black-box multilevel procedure suggested in Reference 4. The proposed method works on a hierarchical sequence of ΓΏnite element meshes to solve the problem with an arithmetic cost, nearly proportional to the dimension of the arising algebraic system. The coarsest mesh in the above sequence of meshes can consist of almost arbitrary triangular patches, which allows in practice to capture the solution even using a moderate number of successive reΓΏnement steps.
The rate of convergence of the algorithm is bounded uniformly with respect to the problem coe cients, namely the Young's modulus E and the Poisson ratio . This makes it possible to apply the method for a broad class of engineering problems.
π SIMILAR VOLUMES
The paper discusses an iterative scheme for solving large-scale three-dimensional linear elasticity problems, discretized on a tensor product of two-dimensional and one-dimensional meshes. A framework is chosen of the additive AMLI method to develop a preconditioner of a `black-box' type which is ro
A Path Integral (PI) formulation of linear elastostatics is "rst presented. For this, Navier equations are modi"ed by adding a "ctitious &time' derivative of displacements so that equilibrium corresponds to the steady state of the resulting di!usion-like equations. The evolution of displacement is t