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A screw dislocation is a crystal defect in which the lattice points lie on a spiral or helical surface that revolves around a center line that is called the dislocation line. A screw dislocation terminates at a crystal surface. Shear stresses are set up in the lattice surrounding a screw dislocation as a result of the distortion in atomic array that the defect causes. The Burgers vector is the distance, measured in multiples of the lattice parameter, that is needed to close a straight-sided loop around a dislocation when going the same number of lattice distances in all four directions. It is the term used to define the size of a dislocation and is designated by the letter b. A characteristic of an edge dislocation is that it lies perpendicular to its Burgers vector, whereas a screw dislocation lies parallel to its Burgers vector.
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32.4.3 Planar Defects There are several types of planar (or surface) defects that occur from a change in the orientation of crystallographic planes across a surface boundary. The most important planar defect is the grain boundary, which is the imperfect plane surface that separates two crystals of different orientation in a polycrystalline solid. Grain boundaries originate when the last few remaining atoms of a liquid freeze onto the meeting faces of two adjacent crystals that have grown from the melt or, similarly, when two adjacent crystals that grow by recrystallization meet each other. The material in the grain boundary is at a higher energy level than the material near the center of the grain because of the increased elastic strain energy of the atoms that are forced from their normal (lowest-energy) sites in a perfect lattice. This higher energy level and lattice distortion cause the grain boundary material to be stronger, have a higher diffusion rate, and serve as a more favorable site for the nucleation of second phases than the interior materials. Another important planar defect is the twin boundary, which is the plane that separates two portions of a single crystal having slightly different orientations. The two twins are mirror images of each other. The distortion of the twinned lattice is low in comparison to that at a grain boundary. Twins which form in most FCC metal crystals, especially the copper- and nickel-base alloys, during freezing from the melt or recrystallization are called annealing twins. Twins which form in some metals during cold work (plastic deformation) are called mechanical twins. A third planar defect is the low-angle grain boundary or low-angle tilt boundary, where the angular misalignment of the two grains is very small, on the order of a few degrees. In a sense it is a very undistorted grain boundary. The angular mismatch of the crystal planes is due to a row of dislocations piled above each other. A stacking fault is a planar defect that occurs when one crystalline plane is stacked out of its normal sequence in the lattice array.The lattice on both sides of the defect is normal. For example, the normal FCC stacking of planes may be interrupted by one layer of a hexagonal close-packed (HCP) plane, since both are closepacked structures with atomic packing factors of 0.74. Such stacking faults can occur during the formation of a crystal or by plastic deformation.
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32.5 SLIP IN CRYSTALLINE SOLIDS
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Slip can be defined as the massive sliding movement of one large body of atoms with respect to the remaining body of atoms of the crystal along crystallographic planes. Slip can also be considered as an avalanche of dislocations along one plane that pile
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Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com) Copyright 2004 The McGraw-Hill Companies. All rights reserved. Any use is subject to the Terms of Use as given at the website.
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