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584  17 Liquid Nonaqueous Electrolytes

                    Table 17.15  (continued)

                    Solid      Liquid          Method     Species          References
                    phase/     phase/
                    electrode  electrolyte

                    Ag, Au, Pt c  LiClO 4 – GBL  FTIR     LiO 2 C(CH 2 ) 2 CH 3 ,  [369, 393]
                                                          β-ketoesterdianion
                    Ag, Au, Pt  LiClO 4 –GBL   FTIR       LiOH,               [393]
                               (H 2 O/O 2 )               LiO 2 C(CH 2 ) 3 OH
                                                          (with water), Li 2 O,
                                                          LiO(CH 2 ) 3 CO 2 Li,
                                                          LiO(CH 2 ) 3 (CO)O 2 Li,
                                                          (with O 2 )
                    Pt c       LiClO 4 –PC     FTIR (in   LiO 2 COR           [369]
                                               situ)
                    Pt         LiClO 4 – THF   Viscosimetry  Living polymers,  [394]
                                                          M ≈
                                                              5
                                                          2 × 10 g·mol −1
                    a Discharged state.
                    b
                     (i) KS44, (ii) Lonza KS6, (iii) Soci´ et´ e des Accumulateurs Fixes et de Traction (SAFT).
                    c 0.3 V vs Li/Li .
                             +
                    For electrolytes which do not show strong ion association, the maxima can be
                    understood on the basis of the defining equation of specific conductivity at the
                    maximum [396], yielding
                          dκ = n e ( dc + cd ) = 0                            (17.47)
                    The maxima are the consequence of two competing effects,

                    • ionic mobilities decreasing with increasing concentration of the salt, and
                    • increasing ionic charge densities.
                      Conductivity equations based on Debye-H¨ uckel-Onsager theory, such as Equation
                    17.9, cannot predict the conductance maxima. They are valuable tools to study dilute
                    solutions in a concentration range below the maximum where the solvent may
                    be described as a homogeneous medium with permittivity and viscosity of the
                    pure solvent compound. For extension of the transport equations in the theory
                    of transport properties, especially the continuity equation approach, the reader is
                    referred to Ref. [183] and the references given there.
                      Theory nowadays overcomes the limitation of concentration range by integral
                    equation and simulation methods. Mean spherical approximation (MSA) and
                    hypernetted chain approximation (HNC) are the most important features yield-
                    ing modern analytical transport equations over extended concentration ranges.
                    Nevertheless, the lcCM expressions maintain their importance. They are reliable
                    expressions for the determination of limiting values of the transport properties
                    at infinite dilution of the electrolyte as a convenient basis for the provision of
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