The Gouy–Chapman law dominates at the low potentials until the potential is such that the distribution of ions in the double layer can no longer be considered Boltzmann and the ‘fermionic’ nature becomes evident.
The Gouy–Chapman law dominates at the lowpotentials until the potential is such that the distribution of ionsin the double layer can no longer be considered Boltzmann andthe ‘fermionic’ nature becomes evident.