Page 21 - Analytical Electrochemistry 2d Ed - Jospeh Wang
P. 21

6                                               FUNDAMENTAL CONCEPTS

              As indicated by equation (1-3), the situation is quite complex when the three
            modes of mass transport occur simultaneously. This complication makes it dif®cult
            to relate the current to the analyte concentration. The situation can be greatly
            simpli®ed by suppressing the electromigration or convection, through the addition of
            excess inert salt or use of a quiescent solution, respectively. Under these conditions,
            the movement of the electroactive species is limited by diffusion. The reaction
            occurring at the surface of the electrode generates a concentration gradient adjacent
            to the surface, which in turn gives rise to a diffusional ¯ux. Equations governing
            diffusion processes are thus relevant to many electroanalytical procedures.
              According to Fick's ®rst law, the rate of diffusion (i.e., the ¯ux) is directly
            proportional to the slope of the concentration gradient:

                                                @C…x; t†
                                     J…x; t†ˆ D                            …1-5†
                                                  @x
            Combination of equations (1-4) and (1-5) yields a general expression for the current
            response:


                                               @C…x; t†
                                      i ˆ nFAD                             …1-6†
                                                 @x
            Hence, the current (at any time) is proportional to the concentration gradient of the
            electroactive species. As indicated by the above equations, the diffusional ¯ux is
            time dependent. Such dependence is described by Fick's second law (for linear
            diffusion):

                                                2
                                    @C…x; t†   @ C…x; t†
                                           ˆ D                             …1-7†
                                       @t        @x 2
            This equation re¯ects the rate of change with time of the concentration between
            parallel planes at points x and (x ‡ dx) (which is equal to the difference in ¯ux at the
            two planes). Fick's second law is valid for the conditions assumed, namely planes
            parallel to one another and perpendicular to the direction of diffusion, i.e., conditions
            of linear diffusion. In contrast, for the case of diffusion toward a spherical electrode
            (where the lines of ¯ux are not parallel but are perpendicular to segments of the
            sphere), Fick's second law has the form

                                            2
                                    @C      @ C  2 @C
                                       ˆ D     ‡                           …1-8†
                                    @t      @r 2  r @r
            where r is the distance from the center of the electrode. Overall, Fick's laws describe
            the ¯ux and the concentration of the electroactive species as functions of position
            and time. The solution of these partial differential equations usually requires the
            application of a (Laplace transformation) mathematical method. The Laplace
            transformation is of great value for such applications, as it enables the conversion
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