Page 49 - Mechanical Behavior of Materials
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50                                      Chapter 2  Structure and Deformation in Materials























            Figure 2.14 The two basic types of dislocations: (a) edge dislocation, and (b) screw
            dislocation. (From [Hayden 65] p. 63; used with permission.)


               Line defects are called dislocations and are the edges of surfaces where there is a relative
            displacement of lattice planes. One type is an edge dislocation, and the other is a screw dislocation,
            both of which are illustrated in Fig. 2.14. The edge dislocation can be thought of as the border of
            an extra plane of atoms, as shown in (a). The dislocation line shown identifies the edge of the extra
            plane, and the special symbol indicated is sometimes used.
               The screw dislocation can be explained by assuming that a perfect crystal is cut as shown
            in Fig. 2.14(b). The crystal is then displaced parallel to the cut and finally reconnected into the
            configuration shown. The dislocation line is the edge of the cut and hence also the border of
            the displaced region. Dislocations in solids generally have a combined edge and screw character
            and form curves and loops. Where many are present, complex tangles of dislocation lines
            may form.
               Grain boundaries can be thought of as a class of surface defect where the lattice planes change
            orientation by a large angle. Within a grain, there may also be low-angle boundaries.Anarrayof
            edge dislocations can form such a boundary, as shown in Fig. 2.15. Several low-angle boundaries
            may exist within a grain, separating regions of slightly different lattice orientation, which are called
            subgrains.
               There are additional types of surface defects. A twin boundary separates two regions of a crystal
            where the lattice planes are a mirror image of one another. If the lattice planes are not in the proper
            sequence for a perfect crystal, a stacking fault is said to exist.


            2.4 ELASTIC DEFORMATION AND THEORETICAL STRENGTH

            The discussion of bonding and structure in solids can be extended to a consideration of the
            physical mechanisms of deformation, as viewed at the size scales of atoms, dislocations, and
            grains. Recall from Chapter 1 that there are three basic types of deformation: elastic, plastic, and
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