Page 43 - Materials Chemistry, Second Edition
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30                                              2 Solid-State Chemistry


                                        (0,0,1)
                                                           (0,1,1)

                                         c


                         (1,0,1)                (1,1,1)
                                             b
                                                      b
                                       a
                                   (0,0,0)                 (0,1,0)
                                           g
                                  a


                           (1,0,0)             (1,1,0)

           Figure 2.9. Illustration of definitive axes and angles for a unit cell. The angles and side lengths shown
           above are not representative of all unit cells; seven types of cell dimensions are possible (see text).

                        Table 2.2. Unit Cell Definitions for the Seven Crystal Systems
           Crystal system           Unit cell vector lengths  Unit cell vector angles
           Cubic (isometric)        jaj¼jbj¼jcj             a ¼ b ¼ g ¼ 90
           Tetragonal               jaj¼jbj 6¼jcj           a ¼ b ¼ g ¼ 90
           Orthorhombic             jaj 6¼jbj 6¼jcj         a ¼ b ¼ g ¼ 90
           Trigonal (rhombohedral)  jaj¼jbj¼jcj             a ¼ b ¼ g 6¼ 90 , g < 120


           Hexagonal                jaj¼jbj 6¼jcj           a ¼ b ¼ 90 , g ¼ 120

           Monoclinic               jaj 6¼jbj 6¼jcj         a ¼ g ¼ 90 , b 6¼ 90

           Triclinic                jaj 6¼jbj 6¼jcj         a 6¼ 90 , b 6¼ 90 , g 6¼ 90

           possesses the same symmetry elements of the bulk crystal, and will generate the
           entire extended crystal lattice via translations along the unit cell axes. The structure
           that exhibits these properties while having the smallest possible volume is referred
           to as the primitive unit cell.
             Figure 2.9 provides a schematic of the defining vectors and angles for a unit cell. It
           is convenient to describe these units as having three vectors (a, b, and c) that may or
           may not be aligned along the Cartesian axes, based on the values of unit cell angles.
           Depending on the geometry and volume of the unit cell, there are seven crystal
           systems that may be generated (Table 2.2).
             For simplicity, fractional coordinates are used to describe the lattice positions in
           terms of crystallographic axes, a, b, and c. For instance, the fractional coordinates
           are (1/2, 1/2, 1/2) for an object perfectly in the middle of a unit cell, midway between
           all three crystallographic axes. To characterize crystallographic planes, integers
           known as Miller indices are used. These numbers are in the format (hkl), and
           correspond to the interception of unit cell vectors at (a/h, b/k, c/l). Figure 2.10
           illustrates examples of the (001), (011) and (221) planes; since (hkl) intercepts the
           unit cell at {(a, b, c) : (1/h,1/k,1/l)}, a zero indicates that the plane is parallel to the
           particular axis, with no interception along  1.  [11]  A Miller index with capped
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