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608  17 Liquid Nonaqueous Electrolytes

                    be determined. Hence the transport of lithium salts in ILs is often observed by
                    pfg-NMR [463, 499, 501].

                    17.4.7.3 Moir´ e Pattern
                    Another nonelectrochemical method was developed by Nishikawa et al., who use
                    the creation of a Moir´ e pattern when two images of a laser beam, which are directed
                    through a diffusion cell, overlap on a screen [502]. Two solutions of different
                    concentrations are brought into contact, resulting in a two-way diffusion. The
                    Moir´ e patterns of ‘blind value,’ that is, the pattern of uniform concentration, and
                    the deviation of this blind value give the local refractive index gradient. With this
                    gradient the concentration profile can be determined and thus, with Fick’s law, the
                    diffusion coefficient. This method has the advantage that local diffusivities can be
                    observed.

                    17.4.7.4 Microelectrodes
                    Electrochemical methods for the determination of diffusion coefficients are not as
                    popular as nonelectrochemical methods. Compared to the number of references
                    with NMR data, the number of diffusion coefficients determined by electrochemical
                    methods is insignificant.
                      The spherical diffusion at microelectrodes [494] with no supporting electrolyte is
                    given by:

                                4nFD ± c
                          I sph =                                             (17.75)
                               πr(1 − t ± )
                    where I sph is the diffusion-limited current density, n the number of electrons, F
                    the Faraday constant, D the diffusion coefficient of the electroactive ion, c the
                    concentration, and t ± the transference number of the electroactive ion.
                      The planar diffusion at macroelectrodes, described by the Cottrell equation [504]

                                    1/2
                                 nFD   c
                          I pl =  1/2  ±  1/2  ,                              (17.76)
                              π  (1 − t ± )t
                    with t the time, can be combined with the spherical diffusion Equation 17.75 to
                    result in the transference number and the diffusion coefficient [494, 505]. Both
                    measurements have to be made to get suitable values.If one of the parameters is only
                    assumed [511], the calculated results cannot be taken as true data. Unfortunately
                    it has to be stressed that the boundary conditions for spherical diffusion are no
                    longer observed if lithium is deposited on the electrode.
                    17.4.7.5 Restricted Diffusion
                    Newman et al. [484] specified a method developed by Harned and French [508],
                    where the relaxation of a concentration gradient is measured in a vertical closed
                    cell, leading to the terminology ‘restricted’ diffusion. The relaxation at long times is
                    observed by determination of the potential difference between reversible electrodes
                    at the end of the cell [510]. The diffusion coefficient can now be calculated from the
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