Abstract

Abstract In this paper, we design two classes of stabilized mixed finite element methods for linear elasticity on simplicial grids. In the first class of elements, we use 𝑯 ⁢ ( div , Ω ; 𝕊 ) ${\boldsymbol{H}(\operatorname{div},\Omega;\mathbb{S})}$ - P k ${P_{k}}$ and 𝑳 2 ⁢ ( Ω ; ℝ n ) ${\boldsymbol{L}^{2}(\Omega;\mathbb{R}^{n})}$ - P k - 1 ${P_{k-1}}$ to approximate the stress and displacement spaces, respectively, for 1 ≤ k ≤ n ${1\leq k\leq n}$ , and employ a stabilization technique in terms of the jump of the discrete displacement over the edges/faces of the triangulation under consideration; in the second class of elements, we use 𝑯 0 1 ⁢ ( Ω ; ℝ n ) ${\boldsymbol{H}_{0}^{1}(\Omega;\mathbb{R}^{n})}$ - P k ${P_{k}}$ to approximate the displacement space for 1 ≤ k ≤ n ${1\leq k\leq n}$ , and adopt the stabilization technique suggested by Brezzi, Fortin, and Marini [19]. We establish the discrete inf-sup conditions, and consequently present the a priori error analysis for them. The main ingredient for the analysis are two special interpolation operators, which can be constructed using a crucial 𝑯 ⁢ ( div ) ${\boldsymbol{H}(\operatorname{div})}$ bubble function space of polynomials on each element. The feature of these methods is the low number of global degrees of freedom in the lowest order case. We present some numerical results to demonstrate the theoretical estimates.

Highlights

  • Assume that Ω ⊂ Rn is a bounded polytope

  • In the early years of this century, Arnold and Winther constructed the first H(div, Ω; S) conforming mixed finite element with polynomial shape functions in two dimensions in [10], which was extended to tetrahedral grids in three dimensions in [1, 4] and simplicial grids in any dimension as a byproduct in [42]

  • The displacement space is approximated by L2(Ω; Rn)-Pk−1 while the stress space is approximated by the space of functions in H(div, Ω; S)-Pk+n−1 whose divergence is in L2(Ω; Rn)-Pk−1 for k ≥ 2

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Summary

Introduction

Assume that Ω ⊂ Rn is a bounded polytope. Denote by S the space of all symmetric n × n tensors. The global degrees of freedom for the stress and the displacement for the stabilized mixed finite element methods are n(n+1) 2

Results
Conclusion

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