Plasticity of zirconium hydrides: a coupled edge and screw discrete dislocation model

Author(s):  
Luca Reali ◽  
Mark R. Wenman ◽  
Adrian P. Sutton ◽  
Daniel S. Balint
2015 ◽  
Vol 82 (1) ◽  
Author(s):  
T.-W. Lin ◽  
G. P. Horn ◽  
H. T. Johnson

Residual stress and crystalline defects in silicon wafers can affect solar cell reliability and performance. Infrared photoelastic measurements are performed for stress mapping in monocrystalline silicon photovoltaic (PV) wafers and compared to photoluminescence (PL) measurements. The wafer stresses are then quantified using a discrete dislocation-based numerical modeling approach, which leads to simulated photoelastic images. The model accounts for wafer stress relaxation due to dislocation structures. The wafer strain energy is then analyzed with respect to the orientation of the dislocation structures. The simulation shows that particular locations on the wafer have only limited slip systems that reduce the wafer strain energy. Experimentally observed dislocation structures are consistent with these observations from the analysis, forming the basis for a more quantitative infrared photoelasticity-based inspection method.


2004 ◽  
Vol 71 (3) ◽  
pp. 433-435 ◽  
Author(s):  
M. X. Shi ◽  
Y. Huang ◽  
M. Li ◽  
K. C. Hwang

The discrete dislocation model is used in this note to investigate the source-limited dislocation generation and glide in nanoindentation. It is shown that once there are enough sources for dislocation generation, the material behavior becomes independent of the dislocation source distribution.


2002 ◽  
Vol 740 ◽  
Author(s):  
Michael J. Starr ◽  
Walter J. Drugan ◽  
Maria d. C. Lopez-Garcia ◽  
Donald S. Stone

ABSTRACTIn a continuation of prior work, a new group of Bragg bubble model experiments have been performed to explore the effects of nanoscale crack size and nanoscale structural geometry on atomically-sharp crack tip dislocation emission behavior. The experiments have been designed to correspond to the theoretical limits that bound the expected crack tip response. Continuum elasticity analyses of these situations have also been carried out, in which the leading-order terms in the Williams expansion (the K and T terms) are determined, and the predictions of these continuum analyses coupled with discrete dislocation theory are compared with the experimental results. The experiments exhibit fascinating changes in crack tip dislocation emission direction with changing crack and structural size, crack location and loading conditions, as well as substantial changes in the magnitude of the resolved shear stress that drives dislocation emission. These changes are predicted well by the continuum elasticity-discrete dislocation model down to extremely small dimensions, on the order of a few atomic spacings. Preliminary experiments were performed with layered and two-atom basis rafts to establish crucial comparisons between theory and experiment that validate the applicability of continuum elasticity theory to make predictions directly related to nanoscale fracture behavior.


Author(s):  
S. Groh ◽  
H. M. Zbib

Discrete dislocation dynamics is a numerical tool developed to model the plasticity of crystalline materials at an intermediate length scale, between the atomistic modeling and the crystal plasticity theory. In this review we show, using examples from the literature, how a discrete dislocation model can be used either in a hierarchical or a concurrent multiscale framework. In the last section of this review, we show through the uniaxial compression of microcrystal application, how a concurrent multiscale model involving a discrete dislocation framework can be used for predictive purposes.


1995 ◽  
Vol 10 (1) ◽  
pp. 183-189 ◽  
Author(s):  
C.C. Huang ◽  
C.C. Yu ◽  
Sanboh Lee

The behavior of screw dislocations dynamically emitted from the tip of a surface crack during loading and unloading has been investigated using a discrete dislocation model. The critical stress intensity factor at the crack tip for dislocation emission is a function of friction stress, core radius of dislocation, and dislocations near the crack tip. During motion, the velocity of dislocation is assumed to be proportional to the effective shear stress to the third power. The effect of crack length and friction stress on dislocation distributions, plastic zone, and dislocation-free zone during loading and unloading was examined.


2012 ◽  
Vol 2012 (0) ◽  
pp. _CM-JP-6-1-_CM-JP-6-7
Author(s):  
Akiyuki Takahashi ◽  
Akihiko Namiki ◽  
Taiki Kogure

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