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ION–SOLVENT INTERACTIONS 147


















                               Fig. 2.49. The five 3d orbitals.


         of factors that make transition-metal ions deviate from the behavior of charged spheres.
         What are these factors?
             In the case of transition-metal ions, the 3d orbitals are not spherically symmetrical;
         in fact, they are as shown in Fig. 2.49. In a gaseous ion (i.e., a free unhydrated ion),
         all the 3d orbitals are equally likely to be occupied because they all correspond to the
         same energy. Now, consider what happens when the ion becomes hydrated by six 36
         water molecules situating themselves at the corners of an octahedron enveloping the
         ion. The lone electron pairs of the oxygen atoms (of the water molecules) exert a
         repulsive force on the valence electrons of the ion (Fig. 2.50).
             This repulsive force acts to the same extent on all the p orbitals, as may be seen
         from Fig. 2.51. The d orbitals, however, can be classified into two types: (1) those that
         are directed along the x, y, and z axes, which are known as the   orbitals, and (2) those
         that are directed between the axes, which are known as the   orbitals. It is clear (Fig.
         2.52) that the repulsive field of the lone electron pairs of the oxygen atoms acts more
         strongly on the   orbitals than on the   orbitals. Thus, under the electrical influence
         of the water molecules  of the primary  solvation sheath,  all the 3d orbitals do not
         correspond to the same energy. They are differentiated into two groups, the  orbitals
         corresponding to a higher energy and the  orbitals  corresponding to a lower energy.
         This splitting of the 3d orbitals into two groups (with differing energy levels) affects
         the heat of hydration and makes it deviate from the values expected on the basis of the
         theory developed earlier in  this chapter,  which neglected  interactions of the water
         molecules with the electron orbitals in the ion.
            Thus, consider a free vanadium ion   and a hydrated vanadium ion. In the case
         of the free ion, all the five 3d orbitals (the two   and the three  orbitals) are equally
         likely to be occupied by the three 3d electrons of vanadium. This is because in the free
         ion, all  five  3d  orbitals  correspond to  the  same energy. In  the  hydrated   ion,

         36
          The figure of six, rather than four, is used because of the experimental evidence that transition-metal ions
          undergo six coordination in the first shell. Correspondingly, the hydration numbers are 10–15.
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