Electrolyte
Debye-Hückel Theory (only valid for dilute solutions)
In electrolyte, the ions are surrounded by clouds of charge opposite their own, due to the attractive forces of the opposing charge. As a result, there is a local excess charge density of one sign opposite to that of the central ion.
The logarithmic mean ionic activity coefficient1 is proportional to the square root of ionic strength2, $\ln f_{\pm}=-A(z_+ z_-)\sqrt{I}$.