scholarly journals A discrete slip plane model for simulating heterogeneous plastic deformation in single crystals

Author(s):  
J. Wijnen ◽  
R.H.J. Peerlings ◽  
J.P.M. Hoefnagels ◽  
M.G.D. Geers
1999 ◽  
Vol 5 (S2) ◽  
pp. 232-233
Author(s):  
D. Juul Jensen

During plastic deformation of typical metals the original grains subdivide. Subdivision by cell formation is a well-known phenomena in metals with medium to high stacking fault energy, but the subdivision may also take place on larger length scales by: i) Formation of single-walled dense dislocation walls (DDWs) and/or double-walled microbands (MBs). The DDWs/MBs are seen as elongated, nearly straight, vertically parallel dislocation boundaries which delineate several cells, thus bounding cell blocks. Typical examples are shown in Fig. 1. ii) Subdivision on a grain scale, for example due to grain-grain interactions or due to the formation of transition bands separating matrix bands. This subdivision is typical for both single crystals and polycrystals. For a general description and recent overview, see [1, 2].The grain subdivision depends on the orientation of the grains. The morphology may appear different in grains of different orientations and the DDW/MBs can be parallel or inclined to a slip plane.


Author(s):  
M.A. Mogilevsky ◽  
L.S. Bushnev

Single crystals of Al were loaded by 15 to 40 GPa shock waves at 77 K with a pulse duration of 1.0 to 0.5 μs and a residual deformation of ∼1%. The analysis of deformation structure peculiarities allows the deformation history to be re-established.After a 20 to 40 GPa loading the dislocation density in the recovered samples was about 1010 cm-2. By measuring the thickness of the 40 GPa shock front in Al, a plastic deformation velocity of 1.07 x 108 s-1 is obtained, from where the moving dislocation density at the front is 7 x 1010 cm-2. A very small part of dislocations moves during the whole time of compression, i.e. a total dislocation density at the front must be in excess of this value by one or two orders. Consequently, due to extremely high stresses, at the front there exists a very unstable structure which is rearranged later with a noticeable decrease in dislocation density.


JOM ◽  
1957 ◽  
Vol 9 (1) ◽  
pp. 136-140 ◽  
Author(s):  
R. S. Davis ◽  
R. L. Fleischer ◽  
J. D. Livingston ◽  
Bruce Chalmers

CrystEngComm ◽  
2021 ◽  
Author(s):  
Benjamin P. A. Gabriele ◽  
Craig J. Williams ◽  
Matthias E. Lauer ◽  
Brian Derby ◽  
Aurora J. Cruz-Cabeza

Nanoindentation measurements in single crystals of carbamazepine form III show that the (020) face is stiffer and harder than the (002) and (101) faces. AFM imaging and molecular simulations reveal that the (020) plane is the most likely slip plane.


1968 ◽  
Vol 39 (11) ◽  
pp. 5145-5149 ◽  
Author(s):  
M. N. Shetty ◽  
J. B. Taylor

2001 ◽  
Vol 42 (9) ◽  
pp. 1998-2002 ◽  
Author(s):  
Koji Hagihara ◽  
Takayoshi Nakano ◽  
Yukichi Umakoshi

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