DISSERTATION
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Results and Discussion<br />
where σm represents the excess charge of the metal and Cd the differential capacitance. This<br />
equation explains that at the pzc the Cd-E curve shows a minimum. In order to find this potential,<br />
we need to evaluate the nature of the differential capacitance and on what parameters it depends.<br />
surface at the potential of zero (free)<br />
charge<br />
σ m = 0<br />
σ i = 0<br />
σ ddl = 0<br />
surface at the potential of zero total<br />
charge<br />
σ m + σ i = 0<br />
σ ddl = 0<br />
surface at any other potential<br />
σ m + σ i + σ ddl = 0<br />
Figure 3.11. Schematic representation of the electrode-electrolyte interface upon<br />
polarization at different potentials. σm, σi and σddl stand for the excess charge in the metal,<br />
compact layer and diffuse double layer, respectively.<br />
3.2 Importance of knowing the surface 42