The distributions of crack border stresses and strains in strain hardening materials under a triaxial stress constmint Tz E [O, OS] are studied. It is found that at 7" = 0 and 0.5, the sin~la~ty of stresses is most serious and coincident with the HRR solution. When 0~ Tz ~0.5, however, the singulari
Elastoplastic three dimensional crack border field—I. Singular structure of the field
✍ Scribed by Wanlin Guo
- Publisher
- Elsevier Science
- Year
- 1993
- Tongue
- English
- Weight
- 957 KB
- Volume
- 46
- Category
- Article
- ISSN
- 0013-7944
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✦ Synopsis
The structure of stress and strain fields at the border of three dimensional cracks in a tension field is investigated for elastoplastic materials treated by a deformation theory. The investigation is based upon the physics of the problem and is conducted with mathematical rigour. It is found that the character of singular stresses is as follows: c,, = rfl+*d,,(O, Tz) (i,j = x,y), where/(z) is a function of triaxial stress constraint Tz. The transverse shear stresses Q,, and cc are of the order of unity. The corresponding in-plane strains E,, (i.j = x, y) have singularity of order n(/(z) -2).
while E,, and E,, are of the order of unity. E,, has the same order as in-plane strains at comer points but may be much weaker in the interior of the crack border. Further, it is argued that the problem can be simplified to a quasi-planar problem with the triaxial stress constraint Tz being considered.
When the solution is degenerated into a plane problem by enforcing the confinement, the exact solution for a plane strain crack is obtained and some interesting phenomena are discussed in detail.
📜 SIMILAR VOLUMES
The general expression for three-dimensional stress distribution around a flat crack under arbitrary loadings is proved and discussed. Conditions under which the expression is valid or invalid are presented. A closed form solution for singular stress field at the intersection of a crack border with