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17.4 Bulk Properties  585

               association constants and related quantities and in general as a suitable source of
               information on the usability of an electrolyte solution for technical application [183].
               MSA is the extension of Debye-H¨ uckel theory to high electrolyte concentrations
               using the same continuum model [397, 398]. Combined with the law of mass
               action for ion- pair formation, MSA-MAL (mass action law approach), and finally
               as associative mean spherical approximation (AMSA) [399–401], it permits us to
               take into account any ion-complex formation. Equations for electrolyte conductivity
               are given by Blum et al. [402, 403]. However, the complexity of battery electrolytes
               hinders the application of a high concentration continuum approach.
                For attempts in the literature to rationalize the maximum, with reference to
               solvation, ion-association, or viscosity of the electrolyte, see Ref. [15].
                The search for a suitable electrolyte requires encompassing studies. It is necessary
               to measure the conductivities of electrolytes with various solvents, solvent mixtures,
               and anions over accessible concentration ranges of the salts, and to cover a
               sufficiently large temperature range and the whole composition range of the binary
               (or ternary) solvent mixture. Figure 17.10 shows an example: the conductivity plot
               of LiAsF 6 in GBL as a function of temperature and molality.
                In the literature, measurements are often given at only 1 mol·kg −1  or 1 mol·L −1
               for some salts in various solvents or mixed solvents. These are not suitable for
               rationalization of results, because the conductivity maxima depend on type of ions,
               solvent, solvent composition, and temperature.
                Results from conductivity measurements can be advantageously evaluated for
               every temperature and solvent composition using a nonlinear fit [404]
                            m               2   a
                           	  
 a
                    κ = κ max   · exp b(m − µ) −  (m − µ)                (17.48)
                             µ                  µ




                   12


                    8

                k  mS cm −1  4


                    0
                     3
                          2
                              1                    330
                             m    0    240  270  300
                                        T
                          mol kg
                               −1
                                        K
               Figure 17.10  Conductivity of LiAsF 6 in GBL as function of temperature T and molality m.
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