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Local Diffusion Convective Impedance

The nonsteady part of the mass balance equation (13.12) may be written as  [Pg.239]

The spatial dependence of the sinusoidal perturbation is evident in the definition [Pg.240]

As contains a dependence on the space coordinates, it is necessary to derive first the local solution. A solution in the form of a series can be obtained as [Pg.240]

For this solution the number of terms that play a role in the series increases with the frequency. Generally the solution given by equation (13.25) is used for the low-frequency solution, and the high-frequency solution is derived by another method. [Pg.240]

with the dimensionless frequency K, - given by equation (13.23). (Taken from Delouis et [Pg.241]


The dimensionless impedance of a small electrode can be defined by summing the effects of die local convective-diffusion impedance, i.e.. [Pg.242]


See other pages where Local Diffusion Convective Impedance is mentioned: [Pg.239]    [Pg.239]    [Pg.1166]   


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