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Exact(48)
The microbands were almost exclusively associated with a single (or primary) {111} glide plane.
These chains are joined by glide plane in double chains through the C(1)–H…O(5) H-bonds (check labeling).
The simulations show cross-slip of screw segments from one (1 1 1) glide plane to another, topological changes, and thermodynamically favorable dislocation reactions.
The initial separation between the screw and the intersecting dislocation on the (1 1 1) glide plane is varied to find a minimum in the activation energy.
The activation energies for cross-slip from the fully glide plane state to the partially cross-slipped state at the 120° intersection forming HL in Ni and Cu are estimated to be ∼0.09 and ∼0.31 eV, respectively.
It is estimated that the activation energies for cross-slip from the fully glide plane state to the partially cross-slipped state at the 120° intersection forming GL in Ni and Cu are ∼0.47 and ∼0.65 eV, respectively, and from the fully cross-slip plane state to the partially cross-slipped state forming LC are ∼0.68 and ∼0.67 eV.
Similar(12)
For two adjacent crystals undergoing single slip, relations between plastic slip rates, slip directions and glide planes are accordingly deduced.
Stereographic projection showed that only those from different Bain groups will have large-angle misorientations between {1 0 0} cleavage planes while dislocation glide planes {1 1 0} usually do not exhibit large-angle misorientation.
This alignment places the crystal glide planes parallel to the planes of (presumed) greatest shearing.
Interactions on intersecting glide planes resulted in junction formation, annihilation, or attractive non-junction-forming configurations, while dislocations on parallel glide planes formed dipoles.
The Haasen model of dislocation generation has been improved by projection of the mechanical stresses on the glide planes.
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