Discrete Dislocations Interacting with a Mode I Crack

1998 ◽  
Vol 538 ◽  
Author(s):  
H.H.M. Cleveringa ◽  
E. Van Der Giessen ◽  
A. Needleman

AbstractSmall scale yielding around a plane strain mode I crack is analyzed using discrete dislocation dynamics. The dislocations are all of edge character, and are modeled as line singularities in an elastic material. At each stage of loading, superposition is used to represent the solution in terms of solutions for edge dislocations in a half-space and a complementary solution that enforces the boundary conditions. The latter is non-singular and obtained from a linear elastic, finite element solution. The lattice resistance to dislocation motion, dislocation nucleation, dislocation interaction with obstacles and dislocation annihilation are incorporated into the formulation through a set of constitutive rules. A relation between the opening traction and the displacement jumps across a cohesive surface ahead of the initial crack tip is also specified, so that crack initiation and crack growth emerge naturally. Material parameters representative of aluminum are employed. Two cases are considered that differ in the strength and density of dislocation obstacles. Results are presented for the evolution of the dislocation structure and the near-tip stress field during the early stages of crack growth.

1999 ◽  
Vol 578 ◽  
Author(s):  
H.H.M. Cleveringa ◽  
E. Van Der Giessen ◽  
A. Needleman

AbstractCyclic loading of a plane strain mode I crack under small scale yielding is analyzed using discrete dislocation dynamics. The dislocations are all of edge character, and are modeled as line singularities in an elastic solid. At each stage of loading, superposition is used to represent the solution in terms of solutions for edge dislocations in a half-space and a nonsingular complementary solution that enforces the boundary conditions, which is obtained from a linear elastic, finite element solution. The lattice resistance to dislocation motion, dislocation nucleation, dislocation interaction with obstacles and dislocation annihilation are incorporated into the formulation through a set of constitutive rules. An elastic relation between the opening traction and the displacement jump across a cohesive surface ahead of the initial crack tip is also specified, which permits crack initiation and crack growth to emerge naturally. It is found that crack growth can occur under cyclic loading conditions even when the peak stress intensity factor is smaller than the stress intensity required for crack growth under monotonic loading conditions.


2020 ◽  
pp. 1-19
Author(s):  
Idoia Gaztelumendi ◽  
H. Villaverde ◽  
B. Pérez ◽  
M. Chapartegui ◽  
S. Flórez ◽  
...  

2004 ◽  
Vol 53 (8) ◽  
pp. 894-899 ◽  
Author(s):  
Kazushi SATO ◽  
Toshiyuki HASHIDA
Keyword(s):  
Mode I ◽  

2006 ◽  
Vol 54 (19) ◽  
pp. 5115-5122 ◽  
Author(s):  
Yasuhide Shindo ◽  
Fumio Narita ◽  
Katsumi Horiguchi ◽  
Tetsu Komatsu

2020 ◽  
Vol 224 ◽  
pp. 106778 ◽  
Author(s):  
J. Manterola ◽  
M. Aguirre ◽  
J. Zurbitu ◽  
J. Renart ◽  
A. Turon ◽  
...  

1996 ◽  
Vol 118 (3) ◽  
pp. 349-355 ◽  
Author(s):  
Cai-Fu Qian ◽  
Ming-O Wang ◽  
Bao-Juan Wu ◽  
Shu-Ho Dai ◽  
J. C. M. Li

Mixed-Mode fatigue crack propagation tests were carried out in stainless-steel cruciform specimens in which a center initial crack oriented at 45 deg was loaded biaxially. When the loadings were in-phase, the crack was deflected with the initial crack growth angles less than 50 deg and when they were out-of-phase, it was branched with the initial crack growth angles larger than 50 deg. In all the cases, the deflected or branched cracks propagated in Mode I, namely ΔKII was almost always zero along the crack paths. The relationship between deflected or branched cracks during propagation was also analyzed.


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