THE PLASTIC DEFORMATION OF THIN COPPER SINGLE CRYSTALS: II. AN ELECTRON MICROSCOPE STUDY OF THE SURFACE STRUCTURE

1967 ◽  
Vol 45 (2) ◽  
pp. 777-786 ◽  
Author(s):  
J. T. Fourie

A comparison is made between the slip-line structure of two copper single crystals, where the glide path length of edge dislocations is 1.44 mm and 0.066 mm, respectively. No significant difference is found. This leads to the conclusion that dislocations that escape at the surface of a crystal are generated very close to it.Stress–strain experiments on thin layers of crystal from the surface and from the center of previously deformed crystals confirm that slip lines are not representative of the bulk deformation. They also show that a flow-stress gradient exists between the surface and the center of the crystal. It is argued that the existence of such a gradient can be used to explain the dependence of the extent of stage I on the glide path length of edge dislocations.


2011 ◽  
Vol 20 (1-3) ◽  
pp. 21-28
Author(s):  
Gerhard Kroeger ◽  
Harald Godon ◽  
Hartmut Neuhäuser

AbstractA transmission electron microscopy (TEM) study of the dislocation structure in slip bands at the Lüders band front in neutron-irradiated copper (Cu) single crystals reveals bands in various stages of development. This permits to specify the dislocation processes in particular for termination of slip band growth in the yield region. The important processes occurring during slip band growth are obstacle destruction by moving dislocations, formation of dynamic pile-ups, frequency of microscopic cross-slip and climb processes, formation of multipoles and of clusters of heavily jogged edge dipoles, which ultimately stop the local deformation in the cleared slip band channel. The formation of a dislocation group in the stress gradient within the Lüders band region is considered and it is shown that the group behaves like a single dislocation placed in the “center of gravity” of the quasi-stationary distribution which is the same as in the static case.







1997 ◽  
Vol 505 ◽  
Author(s):  
Masaodoyama ◽  
Yoshiaki Kogure ◽  
Tadatoshi Nozaki

ABSTRACTDislocations were created near the center of the surface (110) of copper small crystals whose surfaces are (111), (111), (110), (110), (112), and (112) by use of n-body atom potentials and molecular dynamics. At first, a Heidenreich-Shockley partial dislocation was created. As the partial dislocation proceeds, the partial dislocation and the surface was connected with a stacking fault until the next Heidenreich-Shockley partial dislocation was created at the surface.Just before the creation of a partial dislocation the stress was the highest. For larger crystals, forming a step on (110) plane was not enough and a shear was necessary to move dislocations.







1975 ◽  
Vol 25 (1) ◽  
pp. 57-59 ◽  
Author(s):  
S. Okuda ◽  
H. Mizubayashi


2002 ◽  
Vol 82 (16) ◽  
pp. 3129-3147 ◽  
Author(s):  
S. X. Li ◽  
X. W. Li ◽  
Z. F. Zhang ◽  
Z. G. Wang ◽  
K. Lu


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