Open Access Article
Cathryn A.
Hancock
*,
Ai Lien
Ong
and
John R.
Varcoe
Department of Chemistry, Faculty of Engineering and Physical Sciences, University of Surrey, Guildford, GU5 0UW, UK. E-mail: cathrynhancock@hotmail.co.uk; Tel: +44 1483 686838
First published on 23rd June 2014
This ex situ electrochemical study investigates how the oxygen reduction reaction (ORR) on Bi-doped Ca2Ru2O7 pyrochlore catalysts is affected by the addition of carbonate to the aqueous KOH (1 mol dm−3) electrolyte. The parent Ca2Ru2O7 catalyst has been previously reported to be selective towards the generation of CO32− on the reaction of O2 with CO2 (in the presence of H2O) at the cathode of low temperature alkaline polymer electrolyte fuel cells containing alkaline anion-exchange membranes (AAEM): a target is to develop low temperature carbonate fuel cells involving CO32− conduction through the AAEM (for potential CO2 utilisation). Rotating ring disk electrode (RRDE) voltammetry was used to probe the ORR behaviours of Ca2Ru2−xBixO7−y catalysts with x = 0.25, 0.5, 0.75, and 1. The results show that as more Bi was doped into the pyrochlore catalysts, the poorer the on-set potentials compared to the parent Ca2Ru2O7 (which itself yielded a poorer on-set potential to a benchmark Pt black catalyst). Higher levels of Bi-doping tended to reduce n values with higher levels of peroxide generated: all of the pyrochlore catalysts tested gave higher peroxide yields compared to the Pt black benchmark. However, the presence of CO32− in the O2-saturated KOH (1 mol dm−3) electrolyte appeared to improve kinetic performance of the Bi-doped pyrochlore catalysts (the effect being greatest with the x = 0.75 catalyst).
Traditional AFCs/APEFCs operate with OH− cycles: however, an intriguing possibility is to operate APEFCs with CO32− anion cycles, especially as there are reports that AAEMs can conduct CO32− anions with reasonable conductivities of ca. 30 mS cm−1.9 The most debilitating aspect of using the OH− cycles is the degradation of the AAEMs by the OH− ions that are produced via the traditional ORR at the cathode (eqn (1)):
| O2 + 2H2O + 4e− → 4OH− | (1) |
The OH− anions are excellent nucleophiles and can displace the cationic head-groups of the AAEMs (commonly quaternary ammonium groups) via a multitude of degradation mechanisms.10 An AAEM-containing CO32− cycle system, as advocated by Kohl11 and Mustain,2 combats this by replacing the OH− with less nucleophilic CO32− (such that AAEMs that are unstable to OH−-containing electrolytes are chemically stable).3–5 Using the CO3− cycle therefore increases the lifetime of the AAEM and may also improve the hydrogen oxidation reaction (HOR) kinetics at the anode.4
The challenge with developing a CO32− cycle system is the need for an electrode which absorbs CO2 in preference to water in order to generate CO32− selectively over OH− anions on reaction with O2 at the cathode.2–4,12,13 In addition to this, for the cathode catalyst to be effective in a low temperature carbonate fuel cell, it needs to have high electrical conductivity and electrochemical activity to facilitate the electron transfer processes and activate the O2 double bond.14–16 Currently only one CO32− selective catalyst has been reported: the Ca2Ru2O7 (RuV) pyrochlore.2,4,13 The alkaline earth metal on the A site produces a catalyst with a high surface basicity: because CO2 is a stronger Lewis acid than water, this leads to preferential absorption of CO2. The B site introduces a metal with ORR activity in alkaline media, which in this case is Ru.
A low temperature carbonate fuel cell works as shown in Fig. 1. The CO32− anions are produced from the selective reduction of O2 and CO2 at the cathode (eqn (2)). The CO32− anions travel through the membrane (cathode → anode) where they oxidise the H2 at the anode (eqn (3)).11
| Cathode: 2CO2 + O2 + 4e− → 2CO32− | (2) |
| Anode: 2H2 + 2CO32− → 2H2O + 2CO2 + 4e− | (3) |
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| Fig. 1 Schematic for a low temperature carbonate fuel cell. Adapted from Mustain et al.13 | ||
This initial study focuses on the synthesis of Bi-doped Ca2Ru2O7 catalysts, which has been shown in other prior studies to have novel conductivity properties as well as thermal and chemical stability.2,15,16 High surface area Ca2Ru2−xBixO7−y (x = 0, 0.25, 0.5, 0.75 and 1) catalysts were synthesised to determine the effect that the much cheaper Bi (compared to Ru) has on the catalysts' performance and behaviour: this was probed using the rotating ring disk electrode (RRDE) hydrodynamic voltammetry.
The electrolytes used for the RRDE ORR studies were a mixture of an aqueous solution of KOH (1 mol dm−3, analytical grade, Fluka, used as supplied) and K2CO3 (Reagent grade, Fisher) in the following combination of concentrations: KOH (1 mol dm−3) only [for blank experiments], KOH (1 mol dm−3) + K2CO3 (0.01 mol dm−3), KOH (1 mol dm−3) + K2CO3 (0.05 mol dm−3), and finally KOH (1 mol dm−3) + K2CO3 (0.1 mol dm−3). The electrolytes were purged with N2 (99.999%, BOC) for 3 h to ensure the complete removal of CO2 from the solution. Each solution was then separated into 90 cm3 volume samples: one sample was purged with O2 for 1 h to achieve O2-saturation while the other solution was kept O2-free with continued purging with N2. The limited current did not increase further with longer purging times, which indicated O2 saturation was after 1 h of purging.
Once the electrolytes were fully oxygenated, a catalyst-free RRDE (as working electrode) was lowered into each electrolyte solution and the O2 purge pipe was lifted so as to blanket the surface solution with O2 [but not to mechanically disturb the solution (introduce unwanted convection)]. In addition, a reversible hydrogen electrode (Hydroflex RHE, Gaskatel) reference electrode and a Pt wire counter electrode (surface area significantly larger than the area of the RRDE working electrode: length = 50 cm and ∅ = 0.05 cm) were lowered into the solution. Immediately after immersion of the RRDE into each aqueous electrolyte under test, an impedance spectrum (frequency range 180 kHz to 96 Hz, voltage perturbation r.m.s. amplitude = 10 mV) was recorded to determine the uncompensated iR-correction. The background (catalyst-free RRDE) ORR testing was carried out by sweeping the disk potential from +1.00 to −0.30 V vs. RHE at 20 mV s−1: the ring potential was held at +1.2 V vs. RHE at all rotation speeds used for catalyst testing (200, 400, 600, 800, 1200 and 1600 rpm).
Once the catalyst-free Pt-ring GC-disk RRDE was determined to be clean [having a low electron transfer number (n) in the above background tests], the catalyst to be tested was placed on the RRDE as discussed above. Impedance measurements were then repeated with each catalysed RRDE to determine the uncompensated iR-correction required for each test. Initially, cyclic voltammograms were recorded at 50 mV s−1 between the potential limits +1.2 and 0 V vs. RHE in the N2 purged electrolytes for each catalysed RRDE. Following this, the catalysed RRDEs were then placed into the oxygenated electrolytes to perform the ORR measurements in a similar manner to the catalyst-free RRDE background tests: the reduction of O2 was carried out by sweeping the disk potential from +1.00 to −0.30 V vs. RHE at 20 mV s−1: the ring potential was held at +1.2 V vs. RHE. The measurements were repeated for each RRDE and electrolyte at 200 rpm until a stable response was obtained and then further ORR linear sweep voltammograms were recorded with increasing rotation speeds in the range 200–1600 rpm.
m and with the unit cell parameters presented in Table 1. Peaks due to Bi2O3 impurities are present in the x = 0.25 and x = 1 catalysts with the latter highly doped sample containing extensive impurities [hence the unit cell parameters were estimated using the (222) peak at 2θ = 30°]. The broad peaks are indicative of small particle sizes but due to the extreme broadness for the x = 0 sample it was not possible to calculate the unit cell parameter: however, Sato et al. provide unit cell parameters of 10.197(2) with their more crystalline sample yielding sharper peaks (and more accurate cell parameter determinations).17 Using this literature value, the cell volume increases on doping with Bi which is due to the increase in size of the Bi3+ (r = 117 pm, CN = 6) compared to the smaller Ru5+ (r = 70.5 pm, CN = 6).
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| Fig. 2 Powder XRD profiles of the Ca2Ru1−xBixO7−y catalysts synthesised. From top to bottom: x = 0, 0.25, 0.5, 0.75 and 1. | ||
| x | a/Å | Cell volume/Å3 | Particle size/nm |
|---|---|---|---|
| a The cell parameters were taken from literature17 due to the broadness of the XRD peaks. b The cell parameters were estimated from the (222) peak only due to the interferences from the impurities. | |||
| 0 | 10.197a | 1060.27a | — |
| 0.25 | 10.2115(2) | 1064.79(7) | 25 |
| 0.5 | 10.2423(2) | 1074.46(7) | 25 |
| 0.75 | 10.2847(3) | 1087.85(9) | 27 |
| 1 | 10.3142b | 1097.26b | 18 |
For the RRDE method of calculating the electron transfer number, n, it is necessary to determine the collection efficiency of the electrode being used. This is determined experimentally by measuring data using a well-known redox system: in this case the ferrocyanide–ferricyanide system was used (a simple reversible n = 1 e− redox couple). This procedure to calculate collection efficiency has been performed extensively in the past: refer to Fig. 3 in ref. 19.
The (catalyst-free) Pt-ring GC-disk RRDE used in this study had an N value = 41%. N can then be used in eqn (4) and (5) along with the RRDE current data (at a potential of −0.3 V in these experiments) to determine the amount of HO2− yield (%) and the e− (n) per O2 for each catalyst and electrolyte:20
![]() | (4) |
![]() | (5) |
| Concentration of K2CO3/mol dm−3 | n RRDE a | Peroxide yield (%) from RRDEa | n K–L b |
|---|---|---|---|
| a Arithmetic mean and sample standard deviations over all rotations rates. b Koutecký–Levich analyses conducted with the crude assumption that the addition of K2CO3 did not significantly alter the properties of the solution (e.g. O2 solubility, kinematic viscosity etc.). | |||
| 0 | 2.97 ± 0.02 | 51.3 ± 1.0 | 2.14 |
| 0.01 | 3.03 ± 0.03 | 48.7 ± 1.0 | 3.45 |
| 0.05 | 2.95 ± 0.02 | 52.6 ± 1.1 | 3.13 |
| 0.1 | 2.98 ± 0.03 | 51.0 ± 1.2 | 3.12 |
On doping with a small amount of Bi into the pyrochlore catalyst (x = 0.25), no significant difference in the nRRDE values were observed on addition of CO32− into the electrolyte (Fig. 5 and Table 3), while ORR on-set potentials were slightly shifted to less positive values (i.e. higher overpotentials). Both the on-set potentials and the n values were the same as the parent (Bi-free) catalyst for the K2CO3-free electrolyte (Fig. 6) indicating that a small level of Bi doping (x = 0.25) has no significant electrochemical effects. The parent compound has higher (more positive) ORR on-set potentials in the presence of CO32− (0.1 mol dm−3) compared to the x = 0.25 Bi-doped catalyst.
On addition of greater amounts of Bi with the x = 0.5 catalyst, there are visible shifts in the on-set potential to more positive potentials on addition of CO32− (e.g.Fig. 7). The on-set potentials remains at these more positive potentials with the continuing addition of K2CO3 in the electrolyte: this behaviour is different to the parent (Bi-free) system where only the addition of K2CO3 at the smallest 0.01 mol dm−3 concentration led to on-set potentials that were more positive compared to tests with the use of the K2CO3-free benchmark electrolyte. The n values were in general lower than with the Bi-free catalyst but, again, there is no significant increase in the n values with x = 0.5 Bi-doped catalysts on increasing concentrations of K2CO3 (Table 4).
These trends continue for Ca2Ru1.25Bi0.75O6.25 catalyst, which has the greatest shift in on-set potentials on addition of CO32− into the electrolyte of all the catalysts studied (Fig. 8 and Table 5). The improvement in on-set potential on addition of CO32− surpasses that of the prior x = 0.5 Bi-doped catalyst, which again suggests that higher concentrations of K2CO3 in the electrolyte can improve the performances of the higher Bi-doped catalysts (Fig. 9). However, the improved on-set potentials for the x = 0.5 and x = 0.75 Bi-doped catalysts in the presence of CO32− are still less positive than those of the Bi-free parent catalyst in CO32−-free electrolyte: the n values are all lower as well.
The final catalyst studied was the x = 1 sample (that contains significant levels of impurities). Again the on-set potentials shifted to more positive potentials, and the n values only slightly increased, on addition of CO32− (Fig. 10 and Table 6). Interestingly, the on-set potential is better than the previous Ca2Ru1.25Bi0.75O6.25 catalyst in the CO32−-free electrolyte (Fig. 11). However, interferences due to the Bi2O3 impurities cannot obviously be ruled out. Hence, a control experiment with Bi2O3 was conducted. This control experiment showed that Bi2O3 had a better on-set potential than the doped pyrochlore catalyst (Fig. 12): the increased on-set potential of the Ca2RuBiO6 catalyst (compared to Ca2Ru1.25Bi0.75O6.25) may well arise from the Bi2O3 impurities. However when CO32− was added to the electrolyte the on-set potential of the Bi2O3 control catalyst undesirably shifted to less positive potentials (not shown): this may explain why the improvement of on-set potential is less for the x = 1 catalyst compared to the x = 0.75 catalyst on addition of CO32−.
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| Fig. 12 RRDE LSVs of Ca2Ru2−xBixO7−y (x = 0 solid line, x = 0.75 dashed line) and Bi2O3 (dotted line) in O2-saturated aqueous KOH (1 mol dm−3). Rotation rate = 600 rpm. | ||
Due to the Ca2Ru1.25Bi0.75O6.25 catalyst having the best response on addition of CO32− (and the most well defined powder XRD profile with the lease amount of impurities), it was decided to investigate the addition of even greater concentrations of K2CO3. On an increase to 0.5 mol dm−3, the on-set potential and n value did not vary significantly compared to the K2CO3 (0.1 mol dm−3) electrolyte. However there was a significant decrease in current in the diffusion limited region. This indicates significant changes in the properties of the solution and a lowering of the diffusion limited current defined by the Levich equation (eqn (6)):21,22
| iL = 0.62nFADo2/3ω1/2v−1/6Co | (6) |
As well as changing the ionic strength and pH of the solutions (which is why a RHE was used: the measured potentials using a Gaskatel RHE do not change with pH [unlike with the use of other hydrogen-based reference electrodes]), the addition of salts to the electrolyte can cause a decrease in both the O2 concentration and the diffusion coefficient. In conjunction with the rise in kinematic viscosity, this reduces the limiting current of the system. To determine whether the on-set potentials may be significantly affected by addition of too high a concentration of K2CO3, a lower concentration of 0.2 mol dm−3 was additionally tested. Again the on-set potential did not vary significantly, while the limiting current was intermediate between the 0.1 and 0.5 mol dm−3 K2CO3 tests (Fig. 13).
As seen in the Tables of data presented, the e−n value can also been calculated using the Koutecký–Levich equation (eqn (7) – a modified version of eqn (6):
| n = (1/slope)/0.62FD2/3v−1/6CoA | (7) |
485 C mol−1), D = the O2 diffusion coefficient (taken here as = 2.04 × 10−5 cm2 s−1), v = kinematic viscosity (taken here as = 0.01 cm2 s−1), Co = bulk concentration of O2 (taken here as = 7.8 × 10−7 mol cm−3), A = disk area (0.2475 cm2), and the gradient of the slopes are from the plots in Fig. 14 (for the Ca2Ru1.75Bi0.75O6.25 catalyst).
As stated earlier, the values for the various electrolyte parameters (e.g. O2 concentration etc.) are incorrect when K2CO3 is added to the electrolyte (more so with high concentrations): however, this shouldn't affect the values for the K2CO3-free aqueous KOH (1 mol dm−3) electrolyte (where the above values are well established). The reason for the discrepancies between the n values determined from the RRDE method (ratio of ring to disk currents) and K–L analyses may arise from the area A used in eqn (6) and (7). The A used in the calculation is the area of the GC-disk but the powdered catalyst will not fully cover the GC-disk and will cause other uncertainties in A as the catalyst layers will not flat when deposited: hence, the A values will be different for each catalyst with undetermined uncertainties and errors (which is why the RRDE is a preferred method for analysing the response with such catalysts). Further analysis of the data involved the Tafel plots for Ca2Ru1.25Bi0.75O6.25 in O2-saturated aqueous KOH (1 mol dm−3) with different concentrations of K2CO3 (see Fig. 15).23 The Tafel slopes for all concentrations of CO32− are similar. Interestingly, the curves are desirably shifted to the right with increasing concentrations of CO32− (with a plateau at 0.1 mol dm−3). This suggests that either the presence of CO32− enhances the ORR kinetics or that the mechanism or reaction occurring has changed.
Additional experiments were performed on a Pt black catalyst to compare with the parent pyrochlore catalyst. As seen in Fig. 16 the Pt black performs better than the Ca2Ru2O7 in both on-set potential and electron transfer number (Table 7) with the CO32−-free electrolyte. On the addition of the CO32− the electrolyte the on-set potential of the Pt black catalyst decreases (Fig. 17): however, the on-set potential is still significantly greater than that of those of the pyrochlore catalysts. This poorer performance in CO32−-containing solution compared to the CO32−-free solution is also seen with Tafel plots for Pt black (Fig. 18): the CO32−-free electrolyte gives higher ORR kinetic performances and confirms the prior work by Vega et al.1
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| Fig. 16 RRDE LSV comparison of Ca2Ru2O7 (dashed) and Pt black (solid) in O2-saturated KOH (1 mol dm−3) at 600 rpm. | ||
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| Fig. 18 Tafel plots of Pt black in O2-saturated aqueous KOH (1 mol dm−3) with varying concentrations of K2CO3: solid = K2CO3-free and dashed = 0.1 mol dm−3. | ||
This ex situ study shows that such Ca2Ru2−xBixO7−y pyrochlore catalysts have unusual ORR behaviours in aqueous alkali electrolytes in the presence of CO32− anions and this warrants further fundamental studies. Future studies should also investigate the in situ performances of the catalysts in fuel cells with an O2(air)/CO2 mix feeds at the cathode further probe the properties of the catalyst and to investigate if such catalysts operate via carbonate cycles in low temperature carbonate fuel cells containing anion-exchange membranes.
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