๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Dislocation-free zone model of mode III fracture: the effect of crack bluntness

โœ Scribed by Sham-Tsong Shiue; Sanboh Lee


Publisher
Elsevier Science
Year
1994
Tongue
English
Weight
306 KB
Volume
176
Category
Article
ISSN
0921-5093

No coin nor oath required. For personal study only.

โœฆ Synopsis


The effect of crack blunting on mode III fracture is investigated using a discrete dislocation approach. The blunt crack is simulated by a small sharp crack emanating from a semi-elliptic hole. It is found that the applied stress intensity factor for dislocation emission increases with the number of emitted dislocations, but decreases with the increasing extent of bluntness. For a given number of emitted dislocations, the region between the crack tip and furthest dislocation increases with the bluntness of crack. However, the distance between the first dislocation and the crack tip becomes larger as the crack is more blunt. It is implied that the plastic zone and dislocation-free zone sizes increase with the bluntness of the crack. In addition, the dislocation-free zone size also increases with decreasing friction stress. The ductile vs. brittle behavior of the material is also studied. A material with a blunt crack has a lower applied stress intensity factor for dislocation emission, so it behaves more ductile.


๐Ÿ“œ SIMILAR VOLUMES


Distribution function of dislocations an
โœ S.-J. Chang; S. M. Ohr ๐Ÿ“‚ Article ๐Ÿ“… 1983 ๐Ÿ› Springer Netherlands ๐ŸŒ English โš– 145 KB

Recent experimental observations by electron microscopy have shown that a dislocation-free zone (DFZ) is located between the crack tip and a linear distribution of dislocations along the crack plane . The results are generally in support of the elastic-plastic model of fracture with an elastic core

A mixed mode rock fracture model for the
โœ Lewis, R. W.; Koosha, B. ๐Ÿ“‚ Article ๐Ÿ“… 1999 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 182 KB ๐Ÿ‘ 2 views

Crack propagation in rocks is simulated by using a displacement substitution method based on a mixed mode fracture criterion. The main advantage of this model is that it can distinguish between mode I and mode II stress intensity factors simultaneously. A typical finite element program is used to co