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Measure structured deformations

stefan Krömer, Martin Kružík, Marco Morandotti, Elvira Zappale

Abstract

Measure structured deformations are introduced to present a unified theory of deformations of continua. The energy associated with a measure structured deformation is defined via relaxation departing either from energies associated with classical deformations or from energies associated with structured deformations. A concise integral representation of the energy functional is provided both in the unconstrained case and under Dirichlet conditions on a part of the boundary.

Measure structured deformations

Abstract

Measure structured deformations are introduced to present a unified theory of deformations of continua. The energy associated with a measure structured deformation is defined via relaxation departing either from energies associated with classical deformations or from energies associated with structured deformations. A concise integral representation of the energy functional is provided both in the unconstrained case and under Dirichlet conditions on a part of the boundary.
Paper Structure (10 sections, 15 theorems, 141 equations)

This paper contains 10 sections, 15 theorems, 141 equations.

Key Result

Theorem 2.1

Let $G \in L^1(\Omega; \mathbb{R}^{d{\times} N})$. Then there exist a function $f \in SBV(\Omega; \mathbb{R}^{d})$, a Borel function $\beta\colon\Omega\to\mathbb{R}^{d{\times} N}$, and a constant $C_N>0$ depending only on $N$ such that

Theorems & Definitions (37)

  • Theorem 2.1: Alberti Alberti1991, ChoFo97
  • Lemma 2.2: ChoFo97
  • Theorem 2.3: approximation theorem
  • proof
  • Theorem 2.4: integral representation
  • Remark 2.5
  • Remark 2.6
  • Remark 2.7
  • Remark 2.8: Instability of the contribution of $G^s_g$ in $I=J$
  • Proposition 3.1
  • ...and 27 more