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2.3 Electrons in Atoms  •  25

              Figure 2.5                     z                       z                        z
              Orientations and                                                                 p
              shapes of (a) p x ,                                                               z
              (b) p y , and (c) p z                           p
              electron orbitals.     p                        y
                                      x
                                 x                       x                        x

                                                   y                                                y
                                                                             y

                                           (a)                      (b)                     (c)



                                    The number of electron orbitals for each subshell is determined by the third (or
                                 magnetic) quantum number, m l ; m l  can take on integer values between  l and  l, includ-
                                 ing 0. When l   0, m l  can only have a value of 0 because  0 and  0 are the same. This
                                 corresponds to an s subshell, which can have only one orbital. Furthermore, for l   1,
                                 m l  can take on values of  1, 0, and  1, and three p orbitals are possible. Similarly, it can
                                 be shown that d subshells have five orbitals, and f subshells have seven. In the absence
                                 of an external magnetic field, all orbitals within each subshell are identical in energy.
                                 However, when a magnetic field is applied, these subshell states split, with each orbital
                                 assuming a slightly different energy. Table 2.1 presents a summary of the values and
                                 relationships among the n, l, and m l  quantum numbers.
                                    Associated with each electron is a spin moment, which must be oriented either up
                                 or down. Related to this spin moment is the fourth quantum number, m s , for which two
                                                   1
                                                                    1
                                 values are possible: +  (for spin up) and -  (for spin down).
                                                                    2
                                                   2
                                    Thus, the Bohr model was further refined by wave mechanics, in which the intro-
                                 duction of three new quantum numbers gives rise to electron subshells within each shell.
                                 A comparison of these two models on this basis is illustrated, for the hydrogen atom, in
                                 Figures 2.2a and 2.2b.
                                    A complete energy level diagram for the various shells and subshells using the
                                 wave-mechanical model is shown in Figure 2.6. Several features of the diagram are

                                                                            Figure 2.6  Schematic
                                                                            representation of the relative
                                                              f    d
                                                                            energies of the electrons for the
                                                                   p
                                                         f    d
                                                                   s        various shells and subshells.
                                                              p             (From K. M. Ralls, T. H. Courtney, and
                                                     f   d
                                                              s
                                                                            J. Wulff, Introduction to Materials Sci-
                                                         p                  ence and Engineering, p. 22. Copyright ©
                                                    d
                                                         s
                                                                            1976 by John Wiley & Sons, New York.
                                                    p                       Reprinted by permission of John Wiley
                                  Energy            s                       & Sons, Inc.)
                                               d
                                               p
                                               s
                                          p
                                          s
                                     s
                                        1    2    3    4   5    6    7
                                           Principal quantum number, n
   48   49   50   51   52   53   54   55   56   57   58