Abstract
The considerations of Paper I are extended to solve slightly more involved problems in potential distribution, such as line‐plane systems. These simple problems clearly demonstrate some of the methods of the theory of the potential. Their fundamental application to electrolytic systems is considered. The only meaning that can be ascribed to an experimental proof is that the conditions of the computation have been satisfied. The improvement of current distribution in commercial practice is so complex that the theoretical approach can be employed only to present a clear picture of the situation.

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