3.1. Structural Characterization of the Catalysts
XRD analysis was used to investigate the evolution in the crystalline structure of the unsupported catalysts with increasing calcination temperature. The XRD analysis was performed on the calcined catalysts (referred to as “IrO
2-x °C”, where x is the sintering temperature) and on the commercial catalyst (“IrO
2-c”). The corresponding diffraction patterns are shown in
Figure 1. In the commercial and the IrO
2-400°C catalyst, two broad peaks (2θ=35 and 59°) are clearly visible in both XRD patterns. The XRD results for these catalysts are characteristic of materials that are amorphous and/or have small-sized crystallites, while in case of IrO
2-c some additional sharp peaks appear (2θ=40.64, 47.36 and 69°), which are assigned to the metallic Ir. The characteristic peaks of the rutile tetragonal IrO
2 started to develop in the diffraction patterns of the catalysts calcined at 500°C and the peaks were fully developed in the diffraction patterns of catalyst calcined at 600°C. In addition, by increasing the calcination temperature to 500°C, the amorphicity of the electrocatalyst was observed to decrease. After raising the temperature to 600°C, these reflection peaks became thinner and sharper, indicating a higher degree of crystallinity for this material. The XRD pattern also confirmed the absence of other phases, such metallic iridium, which is present in the commercial IrO
2 catalyst.
The Scherrer equation was used to roughly estimate the mean crystal size and the lattice parameter for each IrO
2 electrocatalyst. The IrO
2 reflection peak (101) at 2θ=36° was used to define the full width at half maximum (FWHM) intensity and to calculate crystallite size of IrO
2.The mean crystallite size determined for IrO
2-500 °C is 5 nm, while that for the material obtained at 600 °C is 7 nm. For the amorphous catalysts, the absence of defined diffraction peaks makes it impossible to use the analysis Debye-Scherrer, which meant that the mean crystallite sizes of the materials treated at temperatures at or below 400°C could not be determined. The lattice parameters for the IrO
2 catalysts were determined to be: a=b=4.467 Å and c=3.110 Å for IrO
2-500 °C and a= b=4.457 Å and c=3.140 Å for IrO
2-600 °C material (
Table 1), which are in accordance with the JCPDS database for tetragonal IrO
2-rutile crystallographic pattern (JCPDS No. 15-871).
Transmission electron micrographs for the IrO
2 catalysts are presented in
Figure 2 following the synthesis of these catalysts and before the OER activity evaluation. The presence of aggregates composed of small particles, which are characteristic of unsupported catalysts, are observed in all images. The TEM micrograph of the commercial and IrO
2-400°C catalysts reveal spherical particles with sizes in the 1-2 nm range, but the mean particle size could not be determined due to the agglomeration of these nanoparticles. For the catalysts obtained at IrO
2-500°C and IrO
2-600°C (
Figure 2a–c) spherical morphologies are no longer evident. Furthermore, the particle sizes increase due to coalescence resulting as a consequence of the thermal treatment. Some boundary zones observed for the IrO
2-600°C catalyst are evidence of the majority presence of particles with sizes in the 5-7 nm range, in agreement with the XRD results (
Table 1).
Figure 3a displays the XPS spectra of the Ir4f orbital of all electrocatalysts. Each Ir4f spectrum can be deconvoluted into two sets of doublets, which can be assigned to iridium in different oxidation states. The less intense doublet (the red curve), with 7/2 and 5/2 spin-orbit components located at 61.9 and 65.1 eV, respectively, corresponds to Ir
4+ (IrO
2), while the main doublet, with main components located at 63.8 and 66.9 eV is attributed to IrO
x (x>2). These energy values are consistent with other results reported in the literature [
19,
20] and confirm the absence of metallic iridium (Ir
0), in agreement with in the XRD data. The % percentages of Ir
4+ are 41, 55 and 52% for IrO
2-400 °C, IrO
2-500 °C and IrO
2-600 °C catalysts, respectively. It should be noted that, since XPS is a surface-sensitive technique, the atomic percentages of the Ir
3+ and Ir
4+ components are more accurate for IrO
2-400
oC, because of their smaller particle sizes. For materials with larger particle sizes, the bulk compositions may be somewhat different from those indicated by XPS, because the XPS results do not provide the bulk of these materials. Nevertheless, as electrochemical reactions take place on the surface, it is particularly important to consider the surface state of the catalysts in relation to their electrochemical behavior.
High-resolution oxygen 1s-orbital spectra were also acquired and are displayed in
Figure 3b. Three species are identified at ~530.4 eV, 532.2 eV and 534.2 eV bond energies, attributed to Ir-O and Ir-OH bonds as well as weakly adsorbed molecules of water on their surface, respectively. The latter species do not participate in the stoichiometry of the catalyst and are related to surface adsorbates due to exposure to the atmosphere. Furthermore, the spectra reveals that the O1s orbital shifts to lower energy with increasing calcination temperature. This shift reflects an enhancement in the oxygen content of the oxide form compared to the oxy-hydroxide [
21,
22].
The oxygen to iridium atomic ratios were calculated using the signal intensity from O1s and Ir4f spectra, normalized for the different element sensitivity factor. It was found that the O:Ir ratio is between 2.41 to 2.82 for all three samples, which is slightly higher than the theoretical value of 2 for IrO2, revealing again the co-existence of iridium oxides at higher oxidation states. Furthermore, the O:Ir ratio did not exhibit a specific trend with sintering temperature, indicating that thermal treatment did not result in an oxygen loss on the surface due to the conversion of Ir4+ into Ir3+.
The BET surface areas of the calcined catalysts were determined using nitrogen physisorption isotherms and the BET equation [
19]. The measured BET surface area is characterized by high values and is reduced with calcination temperature. The BET surface area was 185 m
2 g
-1 for IrO
2-400°C, 127 m
2 g
-1 for IrO
2-500°C and reduced to 50% of its initial value (66 m
2 g
-1) when the catalyst was calcined at 600°C. Despite calcination temperature, these values are higher than the reported values in the literature [
14,
20] (32 m
2 g
-1) for commercial IrO
2. It is observed that the modified Adams methods results in the formation of nanosized particles with high surface area. In TEM images, it was shown that the iridium based species grew with calcination temperature. Therefore, the reduction in the BET surface area was sharper when the calcination temperature was increased from 400 to 600°C. This is in agreement with TEM images, where the increase in size of iridium based species had been more evident when the calcination temperature was increased from 400 to 600°C.
3.2. Surface Electrochemistry
Cyclic voltammetry was performed on the calcined catalysts and the commercial IrO
2. During the potential scan, the oxidation states of iridium may change, and thus well-defined current peaks can usually be identified on the studied electrodes.
Figure 4 shows the last cycle of a series of cyclic voltammograms (CVs) for IrO
2-400°C, IrO
2-500°C, IrO
2-600°C and IrO
2-c catalysts recorded at 20mV s
-1 scan rate in 0.5 M aqueous H
2SO
4 at room temperature
. One well defined oxidation reduction peak was observed at about 0.65 V vs Ag/AgCl (more pronounced for the IrO
2-400°C). This redox peak corresponds to the redox reaction of iridium where the oxidation state changes between Ir
3+ and Ir
4+. Additionally, one reduction peak was observed at 1.1 V vs Ag/AgCl which is attributed to the change in the Ir
4+ to Ir
5+ transition. The oxidation peaks for IrO
2-500°C, IrO
2-600°C and IrO
2-c catalysts corresponding to the above oxidation state transitions were not clearly observed. This was most likely due to an overlap with the OER. The OER starts around 1.23 V vs Ag/AgCl where the oxidation peak was supposed to be seen. The recorded current for the CVs decreased with calcination temperature, and it was accompanied by less pronounced redox peaks and smaller surface area under the voltammograms.
The surface area under the voltammograms divided by the scan rate corresponds to the voltametric charge. The oxidation voltametric charges were obtained from CVs over the whole anodic potential window. The charge transferred during the iridium redox reaction is proportional to the number of iridium active sites. It is frequently used as an estimation of electrochemically active surface area (ECSA). The ECSA reduced with the increase of calcination temperature (
Table 2). This was due to the growth of iridium particles with calcination temperature. This result is comparable with the reported BET surface area results, where a similar trend was observed. According to the TEM images, 400-600°C is the temperature range where a major increase in the size of iridium species takes place [
23].
3.3. Activity for the Oxygen Evolution Reaction (OER)
The catalysts’ activities towards the oxygen evolution reaction were evaluated through the polarization curves (LSV measurements) as shown in
Figure 5. The currents in the curves are presented in the form of mass activity (mA/mg Ir). As depicted from this figure, the catalysts‘ performance decreased as the calcination temperature increased. The performance of the commercial IrO
2 is also measured and added to the figure for comparison. The mass activities at 1.5 V vs Ag/AgCl are summarized on the inset table (
Figure 5).
It is evident that the performance of the calcined catalyst (especially IrO
2-400°C) synthesized by Adams method is superior to the commercial IrO
2. The amorphous IrO
2-400°C catalyst is the most active, and its corresponding starting potential of oxygen evolution is the lowest. With the increase of calcination temperature, the starting potential of oxygen evolution increases, since the IrO
2-400°C is more electrocatalytically active (more active sites) than IrO
2-500°C and IrO
2-600°C in OER, resulting in lower current densities at any potential. This decrease to the current (in the performance) with the increase of calcination temperature was due to the reduction in the available ECSA, as previously discussed. This is comparable with the result discussed in surface electrochemistry section, regarding cyclic voltammograms. Moreover, it could be concluded that the amorphous iridium based species have higher activity toward OER compared to crystalline IrO
2 [
16,
19].
To further investigate the OER activity of the catalysts, the OER Tafel slopes for the prepared IrO
2 samples were evaluated in 0.5 M H
2SO
4. For this purpose, the corresponding Tafel plots are shown in
Figure 6. in the voltage range of 1.2-1.45 V vs Ag/AgCl and the calculated Tafel slope for each sample is listed in
Table 3. Tafel slope is an important kinetic parameter to reveal changes in the apparent OER mechanism.
Two Tafel linear regions can be distinguished in these plots, the first one corresponds to slopes close to 60 mV dec
-1 in the low current density regions, and the second with slopes close to 115-118 mV dec
-1 in the higher current density regions for ΙrO
2 400
oC, ΙrO
2 500
oC. Tafel slopes of 40 and 120 mV dec
-1 have been reported for sputtered iridium oxide films and thermally prepared iridium oxides [
16]. The resulting Tafel slopes at low overpotentials deviated slightly from 55 mV dec
-1 obtained for anodically oxidized Ir nanoparticles and are in good accordance with 61 mV dec
-1 obtained for thermally prepared IrO
2 [
24,
25]. However, at higher current densities, a Tafel slope of 120 mV dec
-1 indicates that the rate determining step moves to the oxidative adsorption of water [
5]. Finally, Tafel slopes for ΙrO
2 600
oC, ΙrO
2-c are observed to be higher both of low and high overpotentials and are attributed to the formation of oxides on the surface which is in agreement with the results of XPS analysis.
A single cell PEM water electrolysis cell was used to assess the performance of the synthesized IrO
2 oxides under typical water electrolysis conditions. Each experiment was repeated three times and then characterized using polarization curves. All parameters (ionomer content, cathode, membrane) were kept constant except the calcination temperature of IrO
2 catalyst. Electrolysis performances were measured at a constant temperature of 50°C, at atmospheric pressure (1 bar). Liquid water was fed at the anode with a mass flow rate of 300 g h
-1, while He saturated with vapor (58 kPa H
2O) was supplied at the cathode. The corresponding steady-state polarization curves for all catalyst formulations are shown in
Figure 7. The cell with IrO
2-400°C as anodic electrocatalyst exhibited the highest performance, among all samples, achieving 177 mA cm
-2 at 1.8 V. It should be noted that the reported values are not corrected for the ohmic losses. The superior performance of the MEA with the IrO
2 calcined at 400
oC is in agreement with the findings of the intrinsic OER activity measurements, performed in RDE configuration.
In order to evaluate the stability of the MEAs, short-term testing was carried out for 8 h continuous operation under constant applied potential (1.8 V) and the results are summarized in
Figure 8.
The current density for all MEAs decreased quickly during the first minutes (~50 min) of potential application and then reached a steady-state values during the remaining time of testing. The best-performing MEA, with IrO2-400°C as anode electrocatalyst, showed remarkable stability reaching 200 mA cm-2 after the initial stabilization period. These results are very promising regarding the stability of the synthesized electrocatalysts and MEAs.