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200 CHAPTER 2

            energies of interaction obtained by solving it are then quantized.  Such an approach
            was begun for ion–water interactions by Clementi in the 1970s.
                A quantum mechanical approach to ion–water interactions has the up side that it
            is the kind of development one might think of as inevitable. On the other hand, there
            is a fundamental difficulty that attends all quantum mechanical approaches to reactions
            in chemistry. It is that they concern potential energy and do not account for the entropic
            aspects of the situation. The importance of the latter (cf. the basic thermodynamic
            equation              depends  on temperature, so that at T = 0, the change in
            entropy in  a  reaction,   has  no effect.  However, in  calculations of solvation at
            ordinary temperatures, the increase in order brought about by the effect of the ion on
            the water molecules is an essential feature of the situation. Thus, a quantum mechanical
            approach to solvation can provide information on the energy of individual ion–water
            interactions (clusters in the gas phase have also been calculated), but one has to ask
            whether it is relevant to solution chemistry.
                Another problem in the quantal approach is that ions in solution are not stationary
            as pictured in the quantum mechanical calculations. Depending on the time scale
            considered, they can be seen as darting about or shuffling around. At any rate, they
            move and therefore the reorientation time of the water when an ion approaches is of vital
            concern and affects what is a solvation number (waters moving with the ion) and what is
            a coordination number (Fig. 2.23). However, the Clementi calculations concerned station-
            ary models and cannot have much to do with dynamic solvation numbers.
               Finally, Con way points out that the values of the energies obtained by solving the
            Schrodinger equation and by electrostatics are about the same. But this should be! The
            quantum  mechanical  calculations do  not  infer that the  electrostatic ones (Section
            2.15.11) are wrong. Indeed, the Schrödinger equations solved by Clementi involved
            the same energy that was used in the electrostatic method. It is a matter of whether the
            sophistication of quantization  gives increasing  insight  into  the behavior of a real
            system in solution. The answer in the 1990s is: not yet.
               However,  science evolves!  More will be seen of the quantum mechanical ap-
            proach to solvation and in particular in nonaqueous solutions when there is more
            chance of interactions involving overlap of the orbitals of transition-metal ions and
            those of organic solvent  molecules.  Covalent bond  formation  enters  little into  the
            aqueous calculations because the bonding orbitals in water are taken up in the bonds
            to hydrogen. With organic solvents, the quantum mechanical approach to bonding may
            be essential.
               The trend  pointing to  the  future is  the  molecular  dynamics technique,  and
            treatments of this kind were discussed in Section 2.17. The leaders here are Heinzinger
            and Palinkas (in the 1990’s), and the major thing to note is that the technique provides
            needed information on the number of waters in the first shell. The MD method does
            this by calculating the distribution function (Section 2.17.2) and may also provide
            information on  a second layer,  lifetimes of the solvent molecules in the hydration
            sheath, and so on.
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