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7.5  Slip in Single Crystals  •  223




                          Concept Check 7.1  Which of the following is the slip system for the simple cubic crystal
                          structure? Why?
                                                       5100681109
                                                       5110681109
                                                       5100680109
                                                       5110681119
                          (Note: A unit cell for the simple cubic crystal structure is shown in Figure 3.3.)
                          [The answer may be found at www.wiley.com/college/callister (Student Companion Site).]



              7.5  SLIP IN SINGLE CRYSTALS
                                 A further explanation of slip is simplified by treating the process in single crystals, then
                                 making the appropriate extension to polycrystalline materials. As mentioned previ-
                                 ously, edge, screw, and mixed dislocations move in response to shear stresses applied
                                 along a slip plane and in a slip direction. As noted in Section 6.2, even though an applied
                                 stress may be pure tensile (or compressive), shear components exist at all but parallel
                                 or perpendicular alignments to the stress direction (Equation 6.4b). These are termed
              resolved shear stress  resolved shear stresses, and their magnitudes depend not only on the applied stress, but
                                 also on the orientation of both the slip plane and direction within that plane. Let f rep-
                                 resent the angle between the normal to the slip plane and the applied stress direction,
              Resolved shear     and let l be the angle between the slip and stress directions, as indicated in Figure 7.7;
              stress—dependence   it can then be shown that for the resolved shear stress t R
              on applied stress and
              orientation of stress                        t R = s    cos f  cos l                   (7.2)
              direction relative to
              slip plane normal   where s is the applied stress. In general, f   l   90  because it need not be the case
              and slip direction
                                 that the tensile axis, the slip plane normal, and the slip direction all lie in the same plane.
                                    A metal single crystal has a number of different slip systems that are capable of op-
                                 erating. The resolved shear stress normally differs for each one because the orientation of

                                                            Figure 7.7  Geometric relationships between the
                                              F               tensile axis, slip plane, and slip direction used in
                                                            calculating the resolved shear stress for a single crystal.

                                          A





                                 Normal to
                                 slip plane
                                                     Slip
                                                    direction







                                            F
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