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Current Calculation with OC

The normalised current, that is the gradient G, is given by using matrix V and (9.87). The operation returns gradients at all collocation points, and one just takes the first of these, which refers to X = 0. Alternatively, one can multiply just the top row of V with the concentration vector C, which gives dC/dX X = 0) directly. Note that this is not our usual G yet, because of the way X is normalised here. Regarding (9.77), clearly, [Pg.180]

Alternatively, one can simply work with the X-scaling as it is, and change the analytical solution correspondingly. For example, for the Cottrell experiment, with the usual normalisation, the gradient G at time T has the analytical solution I/VttT (see (2.44) on page 18) while, with the normalisation as used in OC (9.77), the analytical solution for the gradient at the electrode ((2.36, page 16) becomes [Pg.180]

In the case of LSV, however, not dividing by the factor / would lead to currents that are hard to compare with tabled values or values one expects. [Pg.180]


See other pages where Current Calculation with OC is mentioned: [Pg.180]    [Pg.214]   


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