Page 80 - Materials Science and Engineering An Introduction
P. 80

WHY STUDY The Structure of Crystalline Solids?


            The properties of some materials are directly related to   Furthermore, significant property differences exist
            their crystal structures. For example, pure and unde-  between crystalline and noncrystalline materials hav-
            formed magnesium and beryllium, having one crystal   ing the same composition. For example, noncrystalline
            structure, are much more brittle (i.e., fracture at lower     ceramics and polymers normally are optically transparent;
            degrees of deformation) than are pure and undeformed   the same materials in crystalline (or semicrystalline) form
            metals such as gold and silver that have yet another   tend to be opaque or, at best, translucent.
            crystal structure (see Section 7.4).




            Learning Objectives
            After studying this chapter, you should be able to do the following:
            1.   Describe the difference in atomic/molecular   5.   Given three direction index integers, sketch the
               structure between crystalline and noncrystalline   direction corresponding to these indices within a
               materials.                                      unit cell.
            2.   Draw unit cells for face-centered cubic, body-  6.   Specify the Miller indices for a plane that has
               centered cubic, and hexagonal close-packed      been drawn within a unit cell.
               crystal structures.                          7.   Describe how face-centered cubic and hexagonal
            3.   Derive the relationships between unit cell edge   close-packed crystal structures may be generated
               length and atomic radius for face-centered cubic   by the stacking of close-packed planes of atoms.
               and body-centered cubic crystal structures.  8.   Distinguish between single crystals and poly-
            4.   Compute the densities for metals having face-  crystalline materials.
               centered cubic and body-centered cubic crystal   9.  Define isotropy and anisotropy with respect to
               structures given their unit cell dimensions.    material properties.





            3.1    INTRODUCTION
                                Chapter 2 was concerned primarily with the various types of atomic bonding, which are
                                determined by the electron structures of the individual atoms. The present discussion
                                is devoted to the next level of the structure of materials, specifically, to some of the
                                arrangements that may be assumed by atoms in the solid state. Within this framework,
                                concepts of crystallinity and noncrystallinity are introduced. For crystalline solids, the
                                notion of crystal structure is presented, specified in terms of a unit cell. The three com-
                                mon crystal structures found in metals are then detailed, along with the scheme by which
                                crystallographic points, directions, and planes are expressed. Single crystals, polycrys-
                                talline materials, and noncrystalline materials are considered. Another section of this
                                chapter briefly describes how crystal structures are determined experimentally using
                                x-ray diffraction techniques.


            Crystal Structures


            3.2    FUNDAMENTAL CONCEPTS
                                Solid materials may be classified according to the regularity with which atoms or ions
            crystalline         are arranged with respect to one another. A crystalline  material is one in which the
                                atoms are situated in a repeating or periodic array over large atomic distances—that is,
                                long-range order exists, such that upon solidification, the atoms will position themselves

            52  •
   75   76   77   78   79   80   81   82   83   84   85