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On the decomposition of the damage variable in continuum damage mechanics

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Abstract

Refinements and generalizations of the decomposition of the damage variable are presented within the framework of continuum damage mechanics. It is assumed that damage in a solid is due mainly to cracks and voids. The classical decomposition of the damage variable into a damage part due to cracks and another damage part due to voids is examined and extended consistently and mathematically. This is further elaborated upon by considering a solid with three types of defects: cracks, voids, and a third defect that is unspecified. Initially, the decomposition issues are carried out in one dimension using scalars. But this is generalized subsequently for the general case of three-dimensional deformation and damage using tensors. Finally, the special case of plane stress is illustrated as an example. It is shown that in the case of plane stress, two explicit decomposition equations are obtained along with a third implicit coupling equation that relates the various “crack” and “void” damage tensor components.

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Abbreviations

\(\phi \) :

Scalar cross-sectional damage variable

\(\phi ^{c}\) :

Scalar cross-sectional damage variable due to cracks

\(\phi ^{v}\) :

Scalar cross-sectional damage variable due to voids

\(\phi ^{w}\) :

Scalar cross-sectional damage variable due to a third unspecified defect type

\(\varphi _0 \) :

Scalar cross-sectional damage variable due to a single defect type

\(\phi ^{*}\) :

New scalar cross-sectional damage variable

\(\ell \) :

Scalar elastic stiffness degradation damage variable

A :

Cross-sectional area in the deformed/damaged configuration

\({\bar{A}}\) :

Cross-sectional area in the effective/undamaged configuration

\(A^{c}\) :

Cross-sectional area of cracks

\(A^{v}\) :

Cross-sectional area of voids

\(\sigma \) :

Cauchy stress

\({\bar{\sigma }} \) :

Effective Cauchy stress

E :

Elastic modulus in the deformed/damaged configuration

\({\bar{E}}\) :

Effective elastic modulus (in the effective/undamaged configuration)

n :

Number of defect types, with \(n=1, 2, 3, 4, 5 ...\)

[M]:

Matrix representation of fourth-rank damage effect tensor (based on cross-sectional area)

[\(M^{c}\)]:

Matrix representation of fourth-rank damage effect tensor (based on cross-sectional area) due to cracks

[\(M^{v}\)]:

Matrix representation of fourth-rank damage effect tensor (based on cross-sectional area) due voids

[\({M^{w}}\)]:

Matrix representation of fourth-rank damage effect tensor (based on cross-sectional area) due to a third unspecified defect typerth-rank identity tensor

I :

Fourth-rank identity tensor

\(\{\sigma \}\) :

Vector representation of the second-rank stress tensor

\(\{{\bar{\sigma }}\}\) :

Vector representation of the second-rank effective stress tensor

e :

Exponential function

x :

Unknown or unspecified variable

y :

Unknown or unspecified variable

f :

Unknown or unspecified function

[A]:

Exponent matrix that represents a fourth-rank tensor

\(\Delta \) :

Expression related to the second-rank damage tensor

\(\Delta ^{c}\) :

Expression related to the second-rank damage tensor due to cracks

\(\Delta ^{v}\) :

Expression related to the second-rank damage tensor due to voids

\(\phi _{11} , \phi _{22} , \phi _{12} \) :

Components of the second-rank damage tensor

\(\phi _{11}^c , \phi _{22}^c , \phi _{12}^c \) :

Components of the second-rank damage tensor due to cracks

\(\phi _{11}^v , \phi _{22}^v , \phi _{12}^v \) :

Components of the second-rank damage tensor due to voids

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Voyiadjis, G.Z., Kattan, P.I. On the decomposition of the damage variable in continuum damage mechanics. Acta Mech 228, 2499–2517 (2017). https://doi.org/10.1007/s00707-017-1836-1

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  • DOI: https://doi.org/10.1007/s00707-017-1836-1

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