Modelling cracks in finite bodies by distributed dislocation dipoles
The method of continuous distribution of dislocations is extended here to model cracks in finite geometries. The cracks themselves are still modelled by distributed dislocations, whereas the finite boundaries are represented by a continuous distribution of dislocation dipoles. The use of dislocation...
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Published in | Fatigue & fracture of engineering materials & structures Vol. 25; no. 1; pp. 27 - 39 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
Oxford, UK
Blackwell Science Ltd
01.01.2002
Blackwell Science |
Subjects | |
Online Access | Get full text |
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Summary: | The method of continuous distribution of dislocations is extended here to model cracks in finite geometries. The cracks themselves are still modelled by distributed dislocations, whereas the finite boundaries are represented by a continuous distribution of dislocation dipoles. The use of dislocation dipoles, instead of dislocations, provides a unified formulation to treat both simple and arbitrary boundaries in a numerical solution. The method gives a set of singular integral equations with Cauchy kernels, which can be readily solved using Gauss–Chebyshev quadratures for finite bodies of simple shapes. When applied to arbitrary geometries, the continuous distribution of infinitesimal dislocation dipoles is approximated by a discrete distribution of finite dislocation dipoles. Both the stress intensity factor and the T‐stress are evaluated for some well‐known crack problems, in an attempt to assess the performance of the methods and to provide some new engineering data. |
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Bibliography: | ark:/67375/WNG-QP2QWPKC-J ArticleID:FFE440 istex:65E60B30DAB00BA034095401B6961F7BB8B0AB12 ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
ISSN: | 8756-758X 1460-2695 |
DOI: | 10.1046/j.1460-2695.2002.00440.x |