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78 CHAPTER 2

            is short-rangeorder; themolten salts aresomewhatlikeadisordered solution contain-
           ing much open space, which some call holes. However, X-ray analysis does not work
           well for ionic solutions because the ordered elements (solvated ions) turn up only
           occasionally and are interrupted by relatively large distances of disordered solvent
           molecules.
               Although, as will be seen in this section, the developments of neutron diffraction
           during the 1980s (Enderby and Neilson) have led to substantial advances in determin-
           ing the coordination numbers of water molecules around ions, there are still some
           hurdles to clear before one can use this powerful method:
               1. It is necessary to have a neutron source and that, in turn, means that only
                  laboratories that have access to a nuclear reactor can do such work. 18
               2.  It is desirable to  work with  rather  than  because of the  sharper
                  diffraction patterns obtained are the former. This can become a cost burden.
               3.  (1) and (2) can be overcome but the last hurdle is too high and must be accepted:
                  the method is limited (as with most of the spectroscopic methods) to solutions
                                     19
                  of 1 mol    or more,  whereas most of the data in the literature concern
                 dilute solutions (e.g.,  mol  )  where the univalent salts are about 12
                  nanometers apart (one can, then, picture an isolated ion in its solvation shell).
               Having given the obstacles to attainment, let it be said that there are two ways in which
           neutron diffraction can be used to obtain information on the structure around an ion. In the
           first (Soper et al., 1977), the objective is the distribution function in the equation:



           where
               This equation refers to a reference ion  and gives the average  number of
           particles thatexistin aspherical shell ofradius r and thickness dr(of course, on atime
           average). The symbol    is  the  so-called distribution function. For multicompo-
           nent systems, one can generalize   to include all the possible combinations of
           atoms [e.g., NaCl would have a total of 10   values].

            I8
             In U.S. universities, this means that the professor concerned must write a proposal to ask for time on a
             reactor at, for example, Brookhaven or Oak Ridge or Argonne. Such proposals wait in line until they are
             evaluated and then, if accepted, the professor’s team must move to the reactor for some days of intense
             activity—probably shift work to make 24-hr per day use of the time allotted.
            19
             It is easy to show that the average distance between ions in a solution of 1:1 salt is    where
             c is the concentration in mol   For a 1 M solution, this comes to 1.2 nm. However, for an ion of 0.1-
             nm radius and layer of two waters, the radius is about 0.1 + 4  ×  0.16 nm and therefore the internuclear
             distance between two ions in contact is about 1.4 nm. For the   mol   case, the distance apart is
             12.2 nm; i.e., the ions are isolated. Thus, it is very desirable to try to get spectroscopic measurements at
             these dilute  solutions. Only then  can  the results of  spectroscopic  work be  compared  directly  with
             deductions made about solvation (a concentration-dependent property) from measurements of solution
             properties.
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