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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

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