Table of Contents
Fetching ...

A New Div-Div-Conforming Symmetric Tensor Finite Element Space with Applications to the Biharmonic Equation

Long Chen, Xuehai Huang

TL;DR

A new $H(\textrm{divdiv})-conforming finite element is presented, which avoids the need for super-smoothness by redistributing the degrees of freedom to edges and faces, which leads to a hybridizable mixed method with superconvergence for the biharmonic equation.

Abstract

A new $H(\textrm{divdiv})$-conforming finite element is presented, which avoids the need for super-smoothness by redistributing the degrees of freedom to edges and faces. This leads to a hybridizable mixed method with superconvergence for the biharmonic equation. Moreover, new finite element divdiv complexes are established. Finally, new weak Galerkin and $C^0$ discontinuous Galerkin methods for the biharmonic equation are derived.

A New Div-Div-Conforming Symmetric Tensor Finite Element Space with Applications to the Biharmonic Equation

TL;DR

A new $H(\textrm{divdiv})-conforming finite element is presented, which avoids the need for super-smoothness by redistributing the degrees of freedom to edges and faces, which leads to a hybridizable mixed method with superconvergence for the biharmonic equation.

Abstract

A new -conforming finite element is presented, which avoids the need for super-smoothness by redistributing the degrees of freedom to edges and faces. This leads to a hybridizable mixed method with superconvergence for the biharmonic equation. Moreover, new finite element divdiv complexes are established. Finally, new weak Galerkin and discontinuous Galerkin methods for the biharmonic equation are derived.
Paper Structure (25 sections, 38 theorems, 225 equations, 2 figures)

This paper contains 25 sections, 38 theorems, 225 equations, 2 figures.

Key Result

Lemma 2.1

We have for any $\boldsymbol \sigma\in \mathcal{C}^2(T; \mathbb S)$ and $v\in H^2(T)$ that where

Figures (2)

  • Figure 1: Redistribution of vertex degrees of freedom to faces and edges. $\boldsymbol \tau (\texttt{v}_0)\in \mathbb S$ is a symmetric tensor containing $6$ components. Three diagonal entries $\boldsymbol n_{F_i}^{\intercal}\boldsymbol \tau (\texttt{v}_0)\boldsymbol n_{F_i}$ will be distributed to faces $F_i$ for $i=1,2,3$ and three off-diagonal entries $\boldsymbol n_{F_i}^{\intercal}\boldsymbol \tau (\texttt{v}_0)\boldsymbol n_{F_j}$ to the edges $e_{ij} = F_i\cap F_j$ with $1\leq i< j\leq 3$.
  • Figure 2: The lowest degree pair $\Sigma_{1^{++}}(T;\mathbb S) - \mathbb P_1(T)$ in three dimensions.

Theorems & Definitions (70)

  • Lemma 2.1: Lemma 5.2 in ChenHuangDivRn2022
  • Lemma 2.2: Proposition 3.6 in Fuhrer;Heuer;Niemi:2019ultraweak
  • Lemma 2.3
  • proof
  • Lemma 2.4: Theorem 5.10 in ChenHuangDivRn2022
  • Remark 2.5
  • Lemma 2.6
  • proof
  • Lemma 2.7
  • proof
  • ...and 60 more