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122   •  Chapter 4  /  Imperfections in Solids

                                material between these boundaries is appropriately termed a twin. Twins result from
                                atomic displacements that are produced from applied mechanical shear forces (mechan-
                 Tutorial Video:   ical twins) and also during annealing heat treatments following deformation (annealing
                       Defects  twins). Twinning occurs on a definite crystallographic plane and in a specific direction,
                Differences among   both of which depend on the crystal structure. Annealing twins are typically found in
                Point, Linear, and   metals that have the FCC crystal structure, whereas mechanical twins are observed in
                Interfacial Defects
                                BCC and HCP metals. The role of mechanical twins in the deformation process is dis-
                                cussed in Section 7.7. Annealing twins may be observed in the photomicrograph of the
                                polycrystalline brass specimen shown in Figure 4.14c. The twins correspond to those
                                regions having relatively straight and parallel sides and a different visual contrast than
                                the untwinned regions of the grains within which they reside. An explanation for the
                                variety of textural contrasts in this photomicrograph is provided in Section 4.10.

                                Miscellaneous Interfacial Defects
                                Other possible interfacial defects include stacking faults and ferromagnetic domain
                                walls. Stacking faults are found in FCC metals when there is an interruption in the
                                ABCABCABC . . . stacking sequence of close-packed planes (Section 3.12). For ferromag-
                                netic and ferrimagnetic materials, the boundary that separates regions having different
                                directions of magnetization is termed a domain wall, which is discussed in Section 20.7.

                                   Associated with each of the defects discussed in this section is an interfacial energy, the
                                magnitude of which depends on boundary type, and which varies from material to material.
                                Normally, the interfacial energy is greatest for external surfaces and least for domain walls.


                         Concept Check 4.3  The surface energy of a single crystal depends on crystallographic ori-
                         entation. Does this surface energy increase or decrease with an increase in planar density? Why?

                         [The answer may be found at www.wiley.com/college/callister (Student Companion Site).]


            4.7  BULK OR VOLUME DEFECTS
                                Other defects exist in all solid materials that are much larger than those heretofore
                                discussed. These include pores, cracks, foreign inclusions, and other phases. They are
                                normally introduced during processing and fabrication steps. Some of these defects and
                                their effects on the properties of materials are discussed in subsequent chapters.

            4.8    ATOMIC VIBRATIONS
                                Every atom in a solid material is vibrating very rapidly about its lattice position within
            atomic vibration    the crystal. In a sense, these atomic vibrations may be thought of as imperfections or de-
                                fects. At any instant of time, not all atoms vibrate at the same frequency and amplitude
                                or with the same energy. At a given temperature, there exists a distribution of energies
                                for the constituent atoms about an average energy. Over time, the vibrational energy of
                                any specific atom also varies in a random manner. With rising temperature, this average
                                energy increases, and, in fact, the temperature of a solid is really just a measure of the
                                average vibrational activity of atoms and molecules. At room temperature, a typical vi-
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                                brational frequency is on the order of 10  vibrations per second, whereas the amplitude
                                is a few thousandths of a nanometer.
                                   Many properties and processes in solids are manifestations of this vibrational
                                atomic motion. For example, melting occurs when the vibrations are vigorous enough to
                                rupture large numbers of atomic bonds. A more detailed discussion of atomic vibrations
                                and their influence on the properties of materials is presented in Chapter 19.
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