๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Asymptotic analysis of crack interaction with free boundary

โœ Scribed by A.V. Dyskin; L.N. Germanovich; K.B. Ustinov


Publisher
Elsevier Science
Year
2000
Tongue
English
Weight
305 KB
Volume
37
Category
Article
ISSN
0020-7683

No coin nor oath required. For personal study only.

โœฆ Synopsis


This paper employs the beam and dipole asymptotic techniques for modelling interaction of a crack with parallel free boundaries. Two conยฎgurations are considered: (1) a crack in a half-plane and (2) a crack in the centre of an inยฎnite strip. Both, the stress intensity factors and the areas of the crack opening are calculated.

For the crack situated close to the boundary, the part of the material between the crack and the boundary is represented by a beam (plate in plane-strain). This allows calculating the area of the crack opening. The stress intensity factors are calculated by matching the beam approximation with Zlatin and Khrapkov's solution (Zlatin and Khrapkov, 1986) for a semi-inยฎnite crack parallel to the boundary of a half-plane or with Entov and Salganik's solution (Entov and Salganik, 1965) for a central semi-inยฎnite crack in a strip. It has been shown that this asymptotic method allows obtaining two leading terms for the SIFs and the crack opening area.

When the distance between the crack and the free surface is large, the problem is treated in the far ยฎeld approximation. This, dipole asymptotic method allows ยฎnding the leading asymptotic terms responsible for the crackยฑboundary interaction.

For intermediate distances between the crack and the boundary, simple interpolating formulas are derived. Particular examples of cracks loaded by pair of concentrated forces and for uniform loading are considered. The obtained results are compared with available numerical solutions.


๐Ÿ“œ SIMILAR VOLUMES


Analysis of crack-dislocation interactio
โœ M.A. Loyola de Oliveira; G. Michot ๐Ÿ“‚ Article ๐Ÿ“… 1994 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 545 KB

The decrease in stress intensity factor, expected from dislocation emission at a crack tip. can be achieved either through a change in crack tip radius (blunting) or through a crack closure induced by the dislocation (shielding) opposite to the opening imposed by the external stress field. So an app