1994TRANSACTIONS OF THE JAPAN SOCIETY OF MECHANICAL ENGINEERS Series AOpen access

Mathematical Description of Anisotropic Damage State in Continuum Damage Mechanics.

Yuri Nikolaevich Radayev, Sumio MURAKAMI, Kunio Hayakawa

Open full text 2 citations

Abstract

A fictitious equivalent undamaged configuration B*t of an element of a damaged material is first introduced into a three-dimensional Riemannian manifold by excluding the irrelevant rigid rotation of the element. Then a new symmetric damage tensor for three-dimensional anisotropic damage is developed in terms of Finger's tensor of a fictitious deformation gradient from the current damaged configuration Bt to the equivalent undamaged configuration B*t. The damage tensor components are expressed in terms of the metric tensor components of the convective coordinate systems of Bt and B*t. Furthermore, the effective stress tensor of damage mechanics is defined by the equality of stress vectors acting on the damaged and equivalent undamaged plane elements, and the mechanical interpretation of the effective stress tensor and its symmetry condition are discussed. The symmetry condition is also formulated by means of a commutator tensor formed by the tensor pairs : damage tensor-Cauchy stress tensor and damage tensor-reversible gradient. Finally, the symmetrized effective stress tensor is introduced and interpreted.

Open-access reader

About this research paper

What this paper is about

A fictitious equivalent undamaged configuration B*t of an element of a damaged material is first introduced into a three-dimensional Riemannian manifold by excluding the irrelevant rigid rotation of the element. Then a new symmetric damage tensor for three-dimensional anisotropic damage is developed in terms of Finger's tensor of a fictitious deformation gradient from the current damaged configuration Bt to the equivalent undamaged configuration B*t. The damage tensor components are expressed in terms of the metric tensor components of the convective coordinate systems of Bt and B*t. Furthermore, the effective stress tensor of damage mechanics is defined by the equality of stress vectors acting on the damaged and equivalent undamaged plane elements, and the mechanical interpretation of the effective stress tensor and its symmetry condition are discussed. The symmetry condition is also formulated by means of a commutator tensor formed by the tensor pairs : damage tensor-Cauchy stress tensor and damage tensor-reversible gradient. Finally, the symmetrized effective stress tensor is introduced and interpreted.

Why it matters

OpenAlex reports 2 citations for this work. Citation counts describe recorded attention and do not establish research quality.

Key contribution

A contribution statement is not available in the OpenAlex record.

Method / approach

Method details are not available in the OpenAlex metadata.

Main findings

Findings are not separately available in the OpenAlex metadata.

Limitations

Limitations are not available in the OpenAlex metadata.

Applications

Application details are not available in the OpenAlex metadata.

Available abstract

A fictitious equivalent undamaged configuration B*t of an element of a damaged material is first introduced into a three-dimensional Riemannian manifold by excluding the irrelevant rigid rotation of the element. Then a new symmetric damage tensor for three-dimensional anisotropic damage is developed in terms of Finger's tensor of a fictitious deformation gradient from the current damaged configuration Bt to the equivalent undamaged configuration B*t. The damage tensor components are expressed in terms of the metric tensor components of the convective coordinate systems of Bt and B*t. Furthermore, the effective stress tensor of damage mechanics is defined by the equality of stress vectors acting on the damaged and equivalent undamaged plane elements, and the mechanical interpretation of the effective stress tensor and its symmetry condition are discussed. The symmetry condition is also formulated by means of a commutator tensor formed by the tensor pairs : damage tensor-Cauchy stress tensor and damage tensor-reversible gradient. Finally, the symmetrized effective stress tensor is introduced and interpreted.

Key concepts: Viscous stress tensor, Symmetric tensor, Tensor density, Cauchy stress tensor, Tensor contraction, Strain rate tensor, Tensor (intrinsic definition), Cartesian tensor

Related papers

Back to paper searchBrowse research topicsOriginal source
Mathematical Description of Anisotropic Damage State in Continuum Damage Mechanics. — Research Paper | ScholarLens