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Mixed Variational Formulation of Coupled Plates

Jun Hu, Zhen Liu, Rui Ma, Ruishu Wang

Abstract

This paper proposes a mixed variational formulation for the problem of two coupled plates with a rigid {junction}. The proposed mixed {formulation} introduces {the union of} stresses and moments as {an auxiliary variable}, which {are} commonly of great interest in practical applications. The primary challenge lies in determining a suitable {space involving} both boundary and junction conditions of the auxiliary variable. The {theory} of densely defined operators in Hilbert spaces is employed to define {a nonstandard Sobolev space} without the use of trace operators. The well-posedness is established for the mixed formulation. Based on these conditions, this paper provides a framework {of} conforming {mixed} finite element methods. Numerical experiments are given to validate the theoretical results.

Mixed Variational Formulation of Coupled Plates

Abstract

This paper proposes a mixed variational formulation for the problem of two coupled plates with a rigid {junction}. The proposed mixed {formulation} introduces {the union of} stresses and moments as {an auxiliary variable}, which {are} commonly of great interest in practical applications. The primary challenge lies in determining a suitable {space involving} both boundary and junction conditions of the auxiliary variable. The {theory} of densely defined operators in Hilbert spaces is employed to define {a nonstandard Sobolev space} without the use of trace operators. The well-posedness is established for the mixed formulation. Based on these conditions, this paper provides a framework {of} conforming {mixed} finite element methods. Numerical experiments are given to validate the theoretical results.
Paper Structure (12 sections, 7 theorems, 68 equations, 6 figures, 6 tables)

This paper contains 12 sections, 7 theorems, 68 equations, 6 figures, 6 tables.

Key Result

Lemma 2.1

The bilinear form $D(\bullet, \bullet)$ defined in D is continuous and coercive on $W \times W$. Moreover, the solution $\phi$ depends continuously on $F$ with a constant $c$, namely,

Figures (6)

  • Figure 2.1: (A) illustrates the shape and force distribution under the underformed state; (B) and (C) depict the deformed shapes when subjected solely to in-plane and out-of-plane loads, respectively.
  • Figure 2.2: The local coordinate systems of two coupled plates.
  • Figure 4.1: Left and Right are degrees of freedom for a $P_3$-$H(\operatorname{div}, \mathbb{S})$ element and a discontinous vectorial $P_2$ element, respectively.
  • Figure 4.2: Left and Right are degrees of freedom for a $P_4$-$H(\operatorname{divDiv},\mathbb{S})$ element and a discontinous $P_2$ element, respectively.
  • Figure 4.3: The coupled plates with the rigid junction of Example \ref{['ex2']}.
  • ...and 1 more figures

Theorems & Definitions (14)

  • Lemma 2.1: Well-posednesslie1992mathematical
  • Theorem 3.1
  • proof
  • Theorem 3.2
  • proof
  • Theorem 3.3
  • proof
  • Theorem 3.4
  • proof
  • Theorem 4.1
  • ...and 4 more