Softening instability: Part I - localization into a planar band

Zdenek P Bazant*

*Corresponding author for this work

Research output: Contribution to journalConference article

Abstract

Distributed damage such as cracking in heterogeneous brittle materials may be approximately described by a strain-softening continuum. To make analytical solutions feasible, the continuum is assumed to be local but localization of softening strain into a region of vanishing volume is precluded by requiring that the softening region, assumed to be in a state of homogeneous strain, must have a certain minimum thickness which is a material property. Exact conditions of stability of an initially uniform strain field against strain localization are obtained for the case of an infinite layer in which the strain localizes into an infinite planar band. First, the problem is solved for small strain. Then a linearized incremental solution is obtained taking into account geometrical nonlinearity of strain. The stability condition depends on the ratio of the layer thickness to the softening band thickness. If this ratio is not too large compared to 1, the state of homogeneous strain may be stable well into the softening range. Part II of this study applies Eshelby's theorem to determine the conditions of localization into ellipsoidal regions in infinite space, and also solves localization into circular or spherical regions in finite bodies.

Original languageEnglish (US)
JournalAmerican Society of Mechanical Engineers (Paper)
StatePublished - Dec 1 1988
EventPreprint - American Society of Mechanical Engineers - Chicago, IL, USA
Duration: Nov 27 1988Dec 2 1988

ASJC Scopus subject areas

  • Mechanical Engineering

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