Application to large amplitude methods analysis in the Laplace domain

3 Application to large amplitude methods analysis in the Laplace domain 

The most convenient procedure is, instead of combining eqns. (18) and (22), to formulate the Laplace transform of the rate equation, eqn. (18), for constant potential 

As the Laplace transformed current—potential relationship is a much simpler function than its counterpart in the time domain, it has been suggested [76, 77] that it may be advantageous to analyze experimental data in the Laplace domain. In the present case, this would require some procedure to perform Laplace transformation of current datajF(0 i.e. to calculate the integral, according to eqn. (88) 

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