DISSERTATION
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Results and Discussion<br />
In order to find the capacitance minimum in the Cd-E curve, potentiodynamic electrochemical<br />
impedance spectroscopy (PDEIS) was used. This technique consists of a set of EIS<br />
measurements performed for a desired range of potentials. Initially, EIS was performed for all<br />
solutions to identify the suitable frequency range for the determination of the pzc. This was<br />
done to verify whether the system can be fitted to the RC equivalent circuit and that there are<br />
no artifacts in the frequency range of interest. Very high frequencies were excluded since a high<br />
frequency region of the impedance spectra is very sensitive to the cell geometry 79 . To be<br />
specific, the solution resistance is smaller for the electrode edge than for the center of the<br />
electrode, leading to a mixed behavior of the system which cannot be fitted with a simple RC<br />
circuit. In order to minimize this behavior, a setup that assures homogeneous distribution of<br />
current lines was constructed, where the counter electrode completely surrounds the working<br />
electrode and the reference electrode is placed below them (Chapter 5.4, Figure 5.4). Moreover,<br />
very low frequencies were also avoided and with this any possible faradaic side-reactions.<br />
Furthermore, a capacitive bridge (shunt capacitor 80 ) was implemented and a Pb/PbF2 reference<br />
electrode was used that shows high impedance 81 in the measuring setup to eliminate possible<br />
instrumental artifacts due to very low ionic strengths and high frequencies. After these<br />
optimization steps Nyquist plots with the characteristic behavior for a system with the solution<br />
resistance and the double layer capacitance connected in series (Figure 3.13) were obtained. In<br />
an ideal case, a Nyquist plot of this system should consist of a vertical line with the intercepting<br />
the real axis at the solution resistance. However, as shown in Figure 3.13 a frequency dispersion<br />
which is common for polycrystalline electrodes is observed. There are various theories<br />
discussing the reasons for this phenomena, among which are the roughness of polycrystalline<br />
electrodes, that creates inhomogeneities in the current density along the surface, or adsorption<br />
effects 77,82 .<br />
After performing PDEIS for all solutions in the chosen frequency range and the potential range<br />
from -0.2 to 0.7 V (vs. Ag/AgCl/3 M KCl), the determination of Cd was done by extracting the<br />
imaginary impedance component from the Nyquist plots for each sampled potential value and<br />
calculating Cd values using the following equations for the RC equivalent electric circuit:<br />
Z = R −<br />
j<br />
ωC d<br />
(3.3)<br />
3.2 Importance of knowing the surface 44