Electrolysis of CO2 and H2O

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Electrolysis of CO2 and H2O ( electrolysis-co2-and-h2o )

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Chapter 5. Aspects of Metal-YSZ Electrode Kinetics 142 Furthermore, inspecting the chronoamperometry measurements before and the current measured during the potentiostatic IS measurement revealed no correlation between the direction of current drift (if there was any) and the shapes or the impedance spectra (inductive loops or Warburg-like diffusion limitation, including the apparent drift seen for H2O reduction on Pt in Figure 5-22a). Finally, the Kramers-Kronig transform showed very little residual error for nearly all of the impedance measurements (except when there is clearly instability during measurement at high anodic overpotentials). Therefore it is believed that the polarized impedance data, including the inductive loops and diffusion-limitation type responses, is valid. This suggests that adsorbed intermediates play a role in the reaction mechanism for all of the metals and may participate in the rate-limiting step during polarization. 5.3.4.3. Relaxation after Applied Potentials After each set of anodic and cathodic polarized impedance measurements presented in the prior section, the electrode was allowed to rest at OCV and the impedance was monitored (Figure 5-23). In many cases the electrodes were activated (LSRP was decreased) by polarization and a slow relaxation process was observed. Cu. In both H2O/H2O and CO/CO2, the OCV LSRP for Cu was basically unaffected by either anodic or cathodic polarizations (Figure 5-23a+b). Ni. Ni, on the other hand, was activated by anodic polarization in H2/H2O and it took at least 24 hours for the LSRP to relax and return back to near the value before polarization (Figure 5-23c). Activation followed by similar relaxation time constants have been observed for Ni point-contact electrodes [35], as well as porous Ni electrodes [24] and Ni pattern electrodes [22], however the porous and pattern electrodes activated only by <20%, whereas the Ni point electrodes here activated by an order of magnitude. In CO/CO2, Ni was similarly strongly activated (LSRP decreased by more than a factor of 10), however the activation appeared to be more permanent (Figure 5-23d). Returning to H2/H2O seemed to return the LSRP for Ni back to near its ―normal‖ value (not shown). Ni was not significantly affected by cathodic polarization in either atmosphere (Figure 5-23c+d). Pd. In H2/H2O, Pd was strongly activated (LSRP was decreased) by anodic polarization and did not relax much at all and very slowly (Figure 5-23e), similar to Ni in CO/CO2. Cathodic polarization had little effect and even appeared to accelerate the relaxation back to ―normal‖ performance. In CO/CO2, Pd was activated by anodic polarization and fully relaxed after about 24 hours, whereas cathodic polarization caused a more permanent activation, though less than observed for anodic bias of Ni in CO/CO2 and for anodic bias of Pd in H2/H2O. Pt. The anodic polarizations for Pt were only conducted up to +200 mV which may lessen their effects relative to those performed on the other metals which included +300

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