Gibb's phase rule is discussed for the case of immiscible electrolyte solutions. The ways of choosing the independent system variables which are most convenient for the theory of electrocapillarity are described. A simpler description of this section, which will be suited equally well for polarizable interfaces, is formulated.
|Original language||English (US)|
|Number of pages||7|
|State||Published - Sep 1 1988|
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