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ION–SOLVENT INTERACTIONS  83

         molecules in a first shell was 5.85 and the lifetime of these waters was relatively long,
          about       Thus, because this time is much greater than that needed for a diffusive
          movement        the waters in the first shell are certainly a part of the hydration
         number. By analogy with  it  seems likely that the total hydration number is greater
         than this  coordination number because of a  second  shell  containing  water with  a
         lifetime greater than  s,  which would then also qualify (because its lifetime greatly
         exceeds a jump time) as contributing to a hydration number. Similar remarks apply to
             but the lifetime of the inner shell is greater (about 6 ×      s) than that for ferrous
         ions because of the stronger binding to water with ferric rather than ferrous ions.
             The    ion has a special place in the history of solvation because it was the first
         ion for which the lifetime of the water in its hydration shell was measured. This work
         was done by Hunt and Taube in 1957. The exchange of water between the hydration
         shell and the surroundings was slow, so the change in the concentration of the isotope
         could be measured. The lifetime found  is  1.6 ×    s  (about 6  months).  There is
         evidence of outer-sphere water, so the value for the total hydration water that travels
         with the ion  is  much higher  than the  value of about 6  found for the  first  shell in
         transition-metal ions.
             The hydration number of the   ion has been measured by a number of nonspec-
         troscopic methods and a value of 5 ±1 represents the range of results. The difference
         method of neutron diffraction gives 6 with reasonable consistency. The lifetime is 3
         ×     s, so the value is clearly a hydration number (i.e., it is much greater than
         s, so water travels with the ion).
             An interesting result is obtained for   Neutron diffraction work shows the value
         to be 6, which is in strong disagreement with nonspectroscopic methods, which give
         the much lower value of 1  or 2. However, light is at once thrown on what seems a
         breach difficult to mend when the lifetime of the 6 waters around the    is found to
         be only 10 ×        s; this is on the borderline as viable for a dynamic hydration number.
         It seems  likely, then, that the   moves on average without its  hydration  water,
         because its lifetime is barely enough for the time needed  for  wares to travel
         one jump distance. Thus, the  1  or 2 hydration numbers of other measurements is
         understandable. It is possible to regard the 6 value as coordination water, but few of
         the waters manage to stay with the ion when it moves from site to site.

         2.11.4. To What Extent Do Raman Spectra Contribute to Knowledge of
                 the Solvation Shell?
             Raman spectra have a more involved origin than do IR absorption spectra. They
         concern the scattering of light. This is a subject that was studied in the nineteenth
         century when Rayleigh showed that the elastic scattering of light (no absorption) was
         proportional in intensity to   where  is the wavelength of the scattered light. In
         conditions that pertain to the application of this formula,  the photon is  assumed to
         “bounce” off the molecules it strikes with the same energy latterly as it had initially.
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