Page 143 - Materials Science and Engineering An Introduction
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4.5 Dislocations—Linear Defects  •  115



                                                      C Al A Cu
                                             C  Al =             * 100
                                                 C Al A Cu + C Cu A Al
           Tutorial Video:                      =         (97)(63.55 g/mol)      * 100
                  How to                         (97)(63.55 g/mol)  +  (3)(26.98 g/mol)
              Convert from
              Atom Percent                      = 98.7 at%
                 to Weight   and
                  Percent
                                                      C Cu A Al
                                             C  Cu =             * 100
                                                 C Cu A Al + C Al A Cu
                                                          (3)(26.98 g/mol)
                                               =                                 * 100
                                                 (3)(26.98 g/mol)  +  (97)(63.55 g/mol)
                                                = 1.30 at%



              Miscellaneous Imperfections

              4.5   DISLOCATIONS—LINEAR DEFECTS
                                 A dislocation is a linear or one-dimensional defect around which some of the atoms are
                                 misaligned. One type of dislocation is represented in Figure 4.4: an extra portion of a
                                 plane of atoms, or half-plane, the edge of which terminates within the crystal. This is
              edge dislocation   termed an edge dislocation; it is a linear defect that centers on the line that is defined
                                 along the end of the extra half-plane of atoms. This is sometimes termed the dislocation
              dislocation line
                                 line, which, for the edge dislocation in Figure 4.4, is perpendicular to the plane of the
                                 page. Within the region around the dislocation line there is some localized lattice distor-
                                 tion. The atoms above the dislocation line in Figure 4.4 are squeezed together, and those
                                 below are pulled apart; this is reflected in the slight curvature for the vertical planes of
                          : VMSE  atoms as they bend around this extra half-plane. The magnitude of this distortion de-
                           Edge   creases with distance away from the dislocation line; at positions far removed, the crystal
                                 lattice is virtually perfect. Sometimes the edge dislocation in Figure 4.4 is represented by
                                 the symbol #, which also indicates the position of the dislocation line. An edge disloca-
                                 tion may also be formed by an extra half-plane of atoms that is included in the bottom
                                 portion of the crystal; its designation is a  . #
              screw dislocation     Another type of dislocation, called a screw dislocation, may be thought of as being
                                 formed by a shear stress that is applied to produce the distortion shown in Figure 4.5a: the


                                          Burgers vector             Figure 4.4  The atom positions around an
                                              b                      edge dislocation; extra half-plane of atoms
                                                                     shown in perspective.
                                                                     (Adapted from A. G. Guy, Essentials of Materials
                                                                     Science, McGraw-Hill Book Company, New York,
                                                                     NY, 1976, p. 153.)
                                   Edge
                                 dislocation
                                   line
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