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...

Full description

Saved in:
Bibliographic Details
Published inFatigue & fracture of engineering materials & structures Vol. 25; no. 1; pp. 27 - 39
Main Author Dai, D. N.
Format Journal Article
LanguageEnglish
Published Oxford, UK Blackwell Science Ltd 01.01.2002
Blackwell Science
Subjects
Online AccessGet full text

Cover

Loading…
More Information
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.
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