Low-Temperature CO Oxidation
Abstract
Catalytic low-temperature abatement of carbon monoxide becomes essential in environmental pollution control. CO Oxidation, CO Preferential Oxidation (PROX) and Water Gas Shift (WGS) reaction are the conventional technologies used to remove carbon monoxide at low temperature. Perovskite-type oxides have been extensively studied in the last years as catalysts for these reactions due to their high activity and catalytic stability. This chapter describes the state-of-the-art of using perovskite-based catalysts of general formula ABO3 in these reactions. Key factors such as the type and nature of A and B ions or the formation of oxygen vacancies or interstitials by doping are discussed in the light of the reaction mechanism in each case.
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1 Wiley Book title: Perovskites and related mixed oxides Editors: P. Granger et al. LOW TEMPERATURE CO OXIDATION O.H. Lagunaa, L.F. Bobadillab, W.Y. Hernándezc, M.A. Centenoa,* a) Instituto de Ciencia de Materiales de Sevilla. Centro mixto CSIC-Universidad de Sevilla. Avda Americo Vespucio 49. 41092 Sevilla (Spain) Email: [email protected] b) Institute of Chemical Research of Catalonia. Avda. Països Catalans, 16. 43007 Tarragona (Spain) c) Department of Inorganic and Physical Chemistry. Ghent University. Krijgslaan 281, S3, 9000 Ghent (Belgium) Abstract Catalytic low-temperature abatement of carbon monoxide becomes essential in environmental pollution control. CO Oxidation, CO Preferential Oxidation (PROX) and Water Gas Shift (WGS) reaction are the conventional technologies used to remove carbon monoxide at low temperature. Perovskite-type oxides have been extensively studied in the last years as catalysts for these reactions due to their high activity and catalytic stability. This chapter describes the state-of-the-art of using perovskite-based catalysts of general formula ABO3 in these reactions. Key factors such as the type and nature of A and B ions or the formation of oxygen vacancies or interstitials by doping are discussed in the light of the reaction mechanism in each case. Keywords: Perovskite-type oxides; CO abatement, CO oxidation, PROX, WGS reaction; Redox activity; Intrafacial and suprafacial reactions; Oxygen vacancies
2 1. Overview Catalytic oxidation of carbon monoxide at low temperature remains as an intense and important research topic at present considering its impact on environmental, industrial and academic-related studies [1-3]. The interest of CO oxidation deals with the negative influence of such compound over the environment and its high toxicity for the human and animal life. On the other hand, CO poisons the platinum-based catalysts of the proton exchange membrane fuel cells (PEMFC’s), thus being required the abatement of CO from the hydrogen feeding flow at levels below 50 ppm before entering the PEMFC. Consequently, the CO oxidation is a key reaction with a wide range of applications such as trace CO removal in enclosed atmospheres, automotive emission control and H2 clean-up by Water-Gas-Shift (WGS) and CO preferential oxidation (PROX) processes [4-7]. Perovskites (general formula ABO3) are mixed oxides with a well-reported good catalytic activity in CO oxidation reactions at low temperature. Despite that a detailed description of the structural features of perovskites has been presented in previous chapters, some relevant aspects will be briefly summarized below in order to allow an easy understanding of the close relationship between some structural aspects of these materials and their performances in CO oxidation reactions. The catalytic properties of the perovskite-type oxides depend on aspects such as the morphology, the particle size, and the crystalline structure, among others. The chemical composition also results determinant, just as it is the nature of the A and B site ions and their valence state [8]. The A site ions, in contrast to B site ones, are generally proposed to be catalytically inactive although their nature influence the stability of the solid [9, 10]. Nevertheless, substitution of either or both A and B cations with other heterovalent cation or varying the oxygen content of the structure may enhance the catalytic activity due to the formation of structural defects such as cationic or anionic vacancies (e.g., oxygen vacancies) in the network and/or the modification in the oxidation state of the transition metal cation (B-site ion), generating defective or non-
3 stoichiometric oxides without altering the perovskite structure. However, it must be emphasized that there is a limit in the amount of defects that can be accommodated in the perovskite structure and a too large number of vacancies can provoke structural deformations. The non-stoichiometry in perovskites has been widely reviewed and discussed by different authors [11-15]. Recently, in a broad and detailed review about CO oxidation reaction over transition metal oxides, Royer and Duprez [7] remarked the wide number of papers where the effect of the transition metals nature settled in the B position on the perovskite oxides has been studied. In this sense, it is notable the attempt for correlating the catalytic activity for CO oxidation of LaBO3 perovskites (B = V3+, Cr3+, Mn3+, Fe3+, Co3+, or Ni3+) prepared by complexation, with the local symmetry of the solid surface (Figure 1), proposed by Tascon et al. [16]. Figure 1. Specific CO oxidation rate obtained for a series of LaBO3 perovskite solids, plotted as a function of the number of d electrons of the metal ions (conditions of reaction: 0.66 % CO, 0.66 % O2, balance He. Reaction temperature between 373 K and 673 K. (Reprinted from Tascon et al. [16], with permission from Springer) The occurrence of structural and/or valence state modifications are related to the different mechanisms of charge compensation needed to maintain the electro-neutrality of the material’s structure. These effects are proposed to enhance the oxidation catalytic activity of these types of systems either by facilitating oxygen mobility or by enhancing the redox activity of the Bn+ cation [10, 17-19]. Typical examples of such structural
4 modifications on perovskite-related materials have been observed on strontiumsubstituted manganites and ferrites (La1-xSrxMnO3 and La1-xSrxFeO3, respectively). In the case of La1-xSrxMnO3-type materials, the charge modification induced by the presence of Sr2+ in the lattice structure is normally balanced by the oxidation of Mn3+ into Mn4+ [20, 21]. Such situation is favored on substituted manganites since the formation of Mn4+ ions mitigates the static Jahn-Teller distortion of Mn3+ ions [22]. On the other hand, although the presence of Fe4+ ions have been also reported on La1- xSrxFeO3-type materials as a mechanism of charge compensation [19, 23], the formation of oxygen vacancies (on the surface and bulk structure) is the principal way to maintain the electroneutrality of lanthanum-substituted ferrites [23, 24]. The oxygen vacancies influence the ionic and electronic conductivity properties reported for these types of materials [25, 26]. Those structural modifications define the nature of the oxygen species participating in the catalysis at a given temperature reaction. Considering the features of catalysis over perovskite oxides, Voorhoeve et al. [17] introduced the concepts of intrafacial and suprafacial reactions, the former being performed by involving the lattice oxygen of the oxide and the second by means of adsorbed (and/or surface) oxygen species. The suprafacial mechanism prevails in the low temperature range, where the adsorption equilibrium of oxygen is thermodynamically favorable. By increasing the temperature, the surface concentration of adsorbed oxygen decreases, but the lattice oxygen becomes more mobile and so more available, bringing a gradual transition to the intrafacial mechanism. Nevertheless, the concept of suprafacial and intrafacial catalysis is rather empirical and mostly depends on the catalyst’s composition and the nature of the B-site and B-substituting cations. The literature revision presented as follow describes the utilization of perovskite-type materials as CO oxidation catalysts, doing special emphasis on the effect of the materials composition in their catalytic efficiency. Aspects such as the participating oxygen species (adsorbed oxygen and/or bulk-mobile O2- species), surface redox properties and the CO affinity of the considered catalysts will be discussed. 2. Low-temperature CO oxidation reaction Recent excellent papers have reviewed the latest works focused in the applications of perovskites-type oxides for low-temperature CO oxidation [6, 7, 9, 27].
5 Lanthanum-based perovskites containing a transition metal in the B-site (LaBO3, B = Co, Fe, Ni or Mn) have shown catalytic activities close to that of supported-noble metals for such reaction. Nevertheless, most of those perovskites exhibit their highest performances at relatively high temperatures, being their low-temperature activity still far from the well-disperse noble-metal-based catalysts [28]. Doping is usually adopted for preparing perovskites in order to boost their catalytic performance; however, depending on the nature of the dopant ion and its crystallographic position (A and/or B- site partial replacement) diverse catalytic efficiencies and bulk-surface-gas interactions can be achieved. More recently, the utilization of perovskite-type oxides as active supports for noble metals (such as Au and Pd) have gained interest as an alternative to improve the catalyst efficiency of these types of catalyst while maintaining a low noble metal loading [29-31]. This section considers three main families of perovskite-related materials as catalysts for the low-temperature CO oxidation reaction: un-doped ABO3- type perovskites, A, B substituted materials and noble metal-perovskite hybrid materials. 2.1. LaBO3-type perovskites Lanthanum-undoped perovskites are not the most frequently used catalysts for CO oxidation reaction since their catalytic performance is not good enough at low temperatures. Nevertheless, the study of these types of materials represents a good opportunity to differentiate just the effect of the nature of the B-site ion in the catalytic activity and structural properties of the mixed oxide. It has been generally accepted that the catalytic activity of LaBO3 catalysts (B = first-row transition element) is related to its defect nature and density, oxygen adspecies, and reducibility [9]. Among the lanthanum-based perovskites, Mn, Co, and Fecontaining structures has been reported as the most active and promising catalysts for the CO oxidation reaction [32, 33]. The LaCoO3 solid has been extensively studied being proved as catalysts for such catalytic process, obtaining high performances [9, 34, 35]. For these types of catalysts, it is well accepted that the oxidation reaction proceeds according to the suprafacial mechanism: CO first reacts with oxygen adspecies to give CO2, and O2 molecules are activated to be active oxygen adspecies by a B(n+1)+ Bn+
6 redox process [35]. Thus, a high redox activity of the B-site ion will facilitate the activation and stabilization of surface oxygen species (denoted as -O2 from TPD-O2 measurements) during the reaction. Levasseur et al. [36] studied and compared the reducibility of LaMnO3, LaCoO3 and LaFeO3 perovskites synthesized by reactive grinding. The H2-TPR profiles showed that, on LaCoO3 and LaFeO3 materials, B3+-site ions were able to be totally reduced, up to the metallic state (M0), while the reducibility of Mn in LaMnO3 material stops at the Mn2+ state. For all the analyzed materials, the first step of reduction (Bn+ to B2+) occurs at temperatures below 500 ºC (Figure 2). Concerning the LaMnO3 solid, the presence of a low temperature reduction peak (as a shoulder) and a higher H2 consumption above 0.5 mol of H2 per B atom, were clear evidences of the presence of Mn4+ cations. Similar results were reported by Liu et al. [35] on LaMnO3 and LaCoO3 perovskites with a typical hollow spherical morphology. Figure 2. H2-TPR profiles of LaBO3 perovskites (Reprinted from Levasseur et al. [36], with permission from Elsevier) From XPS analyses, the coexistence of Mn4+ and Mn3+ species was evidenced in LaMnO3 material, while the LaCoO3 one showed the presence of Co3+ and Co2+ at the same time. Additionally, these authors established a higher Oads/Olatt molar ratio on LaCoO3 perovskite than that observed for the LaMnO3 one. This phenomenon, observed at the surface of the material, along to improve the low-temperature reducibility of LaCoO3 material, where the catalyst’s properties claimed to be responsible of the remarkable catalytic performance of the cobalt-based perovskite for the CO oxidation reaction. Other authors have also remarked the importance of the presence of Co3+ species as active sites for the adsorption of CO [37-39]. For instance, by using DRIFT spectroscopy, Natile et al. [37] showed that the reactivity of LaCoO3 powders respect to
7 carbon monoxide occurs through the Lewis acidic sites distributed on the surface of the sample, that is, Co3+ species, while oxygen is preferably adsorbed as molecular O2- species on Co2+ ions. This behaviour can also explain the improved capacity of cobaltites-type perovskites as CO oxidation catalysts compared with manganite and ferrite ones. LaFeO3 perovskites have also been reported as catalysts for the CO oxidation reaction [40, 41]. Although their catalytic performance at low temperatures was not as good as those reported for LaCoO3 and LaMnO3 catalysts, some improvements have been obtained by modifying their textural and morphological properties through different synthetic routes. Using a nanocasting strategy with mesoporous silica (KIT-6) and SiO2 nanospheres as hard template, Deng and coworkers [40] prepared wormholelike mesoporous LaFeO3 with a high surface area (up to 138 m2/g). The catalytic activity of such material for the CO and toluene oxidation reactions was improved, compared with that of the bulk material. In fact, the mesoporous material showed a significant increase in the surface Oads/Olatt molar ratio (3.42) in comparison to that of the LaFeO3-bulk (1.07) as well as a high concentration of Fe4+ species. Those material’s features along with a strong redox capability of the perovskite guarantees the occurrence of the suprafacial mechanism where the CO reacts with the oxygen adspecies, while gas phase oxygen is activated by the Fe4+/Fe3+ redox cycle. On the other hand, by using a non-aqueous preparation route, Yang and coworkers [41] reported the synthesis of a nanocrystalline LaFeO3 perovskite. Improved oxygen mobility was observed in the nanostructured material by temperatureprogrammed oxygen isotopic exchange (TPOIE). During the oxidation of CO it was concluded that the higher mobility of oxygen on the surface or even the subsurface as well as a better surface Fe3+ redox capacity were favorable for the reaction. Actually, these authors have proposed that CO oxidation reaction on the nano-LaFeO3 proceeds through a redox surface oxidation mechanism in which surface oxygen from the solid is consumed, rather than through a pure suprafacial mechanism.
8 2.2. La1-xAxB1-yB’yO3-type perovskites The partial replacement of host A cations in ABO3 perovskite-type structures by foreign A ones having a different valence, induces several electronic and ionic defects in the bulk of these materials (e.g. generation of oxygen vacancies), affecting their catalytic properties. A similar scenario may be generated by means of the partial substitution of B-site ions, but mixing two different B-site components, being both catalytically active, can often produce a strong synergetic effect, observed in the catalytic oxidation capacity of the materials. Among the substituted perovskites used as catalysts for the CO oxidation reaction, the La-based ones are the most popular systems reported in the literature [10, 17, 18, 42, 43]. In general, the partial replacement of La3+ with cations of other elements with lower oxidation states (such as Sr2+, Ba2+ or Ca2+) increases the concentration of oxygen vacancies in the materials structure (favoring their oxygen adsorption/activation capacity) and/or favors the increment in the average oxidation state of the cation in position B (improving the redox properties). Both situations are beneficial for the low temperature CO oxidation activity of these types of catalytic systems. On the other hand, the partial replacement of the B-site ion by other redox-active transition metal ones was also reported as an efficient way to improve the CO oxidation capability of these types of materials [10, 44, 45]. Different B-site combinations have been explored by using the most active metal transition ions reported, i.e. Co, Mn, Fe. In general it is accepted that the presence of a second ionic transition metal facilitates the electronic transport during the catalytic redox cycle, which also enhances the material’s reducibility. Besides, the combination of Co, Mn and Fe with Cu in the perovskite structure has shown a very strong influence on the catalytic oxidation properties of these materials [46, 47]. 2.3. Noble metal-perovskite hybrid materials As mentioned above, one of the principal aims of using perovskites-type oxides as oxidation catalysts is to avoid the use of expensive and low-thermally stable noblemetal supported catalysts (e.g. Pt/Al2O3). Thus, by modification of the perovskite
9 composition using alkaline earth metal or metal transition cations (A and/or B substituted materials) and by improving their textural and defective properties during the synthesis process, it is possible to obtain perovskite-based catalysts as active as noble metal supported ones for the low-temperature CO oxidation reaction. Nevertheless, some authors have recently claimed the utilization of these types of mixed oxides as active supports for the deposition of gold nanoparticles, constituting a very efficient low-temperature CO oxidation catalyst [31, 48, 49]. It is well known that dispersed gold nanoparticles on active supports (such as TiO2, CeO2 and Fe2O3) constitute a family of catalysts highly active in this reaction [50-52]. Besides the gold particle size, the choice of an adequate support plays a decisive role in the activation of the gas phase molecules during the oxidation reaction, as well as the stabilization of the gold-active species [51]. In this sense, considering that perovskite oxides exhibit good stability, highly anti-poisoning ability and high catalytic performance in the CO oxidation process, their using as supports for gold nanoparticles have been proved because it is an excellent way to obtain materials with enhanced catalytic activity and stability. Dai et al. [31, 48, 49] have studied the performance of these types of catalysts, focusing their attention on the effect of the perovskite composition and gold loading. In addition, these authors have also proposed the utilization of perovskite supports characterized by a three dimensional macroporous ordered structure (3DOM materials), as a way to improve the surface area of these types of materials, the presence of defects (as oxygen activating centers) and the diffusion of the gas molecules. In fact, for all the perovskites studied, i.e. LaMnO3 [48], LaCoO3 [49] and La0.6Sr0.4MnO3 [31], the utilization of 3DOM-structured materials showed a positive effect by itself on the CO oxidation reaction (Figure 3).
16 ions or even by vacancies and involves diffusion of oxygen ions through the lattice with the formation of neighboring high valence metal ions. β-oxygen is observed for both substituted and unsubstituted samples; the O diffusion inside the lattice is accompanied by the A and/or B ionic diffusion and, therefore, it is activated at higher temperatures than α-oxygen [73]. It is likely that these β-oxygen species could take part in the WGS reaction to increase catalyst activity at high temperatures. Besides the direct use of perovskites as catalysts for the WGS, these materials have been explored as noble metals support, obtaining highly active catalytic systems. Particularly, precious metals supported on LaBO3 perovskites have been recently described as very promising catalysts for the low temperature WGS. Jijil et al. [74] reported the use of platinum doped barium cerate as catalysts for WGS reaction. They found a maximum CO conversion at 350 ºC and observed that the oxygen vacancies population of the system increase with the Pt substitution. Similar results were reported by Rajesh et al. [75] who investigated the doping of BaCeO3 perovskite with different amounts of Pt for the WGS reaction and they found that ionic Pt species are stabilized in lattice points of the BaCeO3 structure increasing the oxygen vacancies of the material as increasing the Pt incorporation. From here, BaCeO3 was proposed to be an ideal perovskite lattice to stabilize ionic Pt, maintaining it not only active but also avoiding its sintering under WGS conditions. The same authors investigated the role of oxygen vacancies in WGS reaction on BaCeO3 perovskite co-doped with platinum and yttrium [76], concluding that the controlled addition of yttrium allows to tailor the oxygen vacancies concentration in the material, as a consequence of the Y(III) to Ce(IV) substitution. Structural and activity studies reveal that the compound with a 6% Y in its composition has the most symmetric B site coordination environment and exhibits the highest WGS activity (Figure 4). Hence, a dependence of the activity with the crystallographic characteristics of the perovskite more than on the concentration of oxygen vacancies is proposed. Symmetric coordination around B ions facilitates water adsorption and dissociation by lowering the energy barriers due to the creation of an isotropic environment. On the other hand, the oxygen vacancies act as water activation centers, favoring the dissociation of the water molecule and generating an oxide/hydroxide ion on the surface. This indicates an important role played by oxygen vacancies in WGS
17 reaction. Similar conclusion has been clearly demonstrated for Au/CeO2 WGS catalysts [77], where the decisive role played by the oxygen vacancies in the water activation procedure has been evidenced. Sekine et al. [78] investigated the WGS reaction at low temperature (300 ºC) over Pt and Pd catalysts supported on several LaBO3 (B = Cr, Mn, Fe, Co and Ni) perovskite oxides prepared using the Pechini method. They observed that perovskite oxides without active metal showed no activity for the WGS reaction while those loaded with Pt and Pd exhibited good WGS activity. Interaction between Pt or Pd and the support promotes the WGS reaction. They found that both Pt/LaCoO3 and Pd/LaCoO3 catalysts have high catalytic activity, although Pt/LaCoO3 catalyst deactivated immediately, and Pd/LaCoO3, although initially less active, exhibited superior stability. The cause of deactivation of Pt/ LaCoO3 was attributed to the reduction of Co and Pt cations. Figure 4. Specific activity of BaCe0.98–xYxPt0.02O3−δ under WGS conditions: (■) x = 0, (●) x = 0.02, (▲) x = 0.04, (▼) x = 0.06, (◀) x = 0.10, (▶) x = 0.20, and (◆) = 0.30. Reformate composition: 40.3% H2, 35.1% N2, 10.1% CO, and 14.5% CO2 with a steam to CO ratio of 4.5 and GHSV of 5000 h–1. (Reprinted with permission from T. Rajesh et al. [76]. Copyright 2014 American Chemical Society) Recently, Rajesh et al. [79] studied the oxidation state of Pt incorporated in perovskites LaBO3 (B = Mn, Co, Fe) for WGS activity. They observed that Pt doped Mn-perovskite showed very poor activity likely attributed to the sintering of Pt particles
18 on the surface, while Pt doped Co and Fe perovskite catalysts showed almost 90% CO conversion above 300ºC. XPS measurements indicate that Pt could be stabilized in ionic form in Co and Fe perovskites but not in LaMnO3 one. This result suggests a possible key influence of the oxidation state of Pt as well as of the enhanced presence of oxygen vacancies in the doped samples, in the activity. It is possible that ionic Pt species in tandem with oxygen vacancies capable of acting as water adsorption and activation sites may enhance the WGS activity of the perovskite. In other study, the same authors synthesized Pt doped LaMnO3 perovskites [80]. Characterization studies evidenced that a structure with an oxygen excess, as LaMnO3, presented a substantial resistance to B site doping with Pt. This behavior was different from other oxygen deficient perovskites, such as LaCoO3 and LaFeO3, in which the lattice was able to stabilize the active species against sintering. In doped samples, a strong interaction of Pt species with a persistent amorphous phase prevents the sintering, enhancing the activity when compared with impregnated sample. The study revealed a possible mechanism in which only metallic Pt species were active, with the perovskite oxide playing a minimal role in the system due to the resistance to lattice incorporation. The authors concluded that crystalline PtOx species were not as active as Pt0 for WGS reaction. 3.2. Perovskites for the preferential CO oxidation in the presence of H2 (PROX) Only few reports are specifically devoted to the preferential oxidation of CO in presence of H2 in the open literature. However, since this reaction is very close to the oxidation of CO in the absent of hydrogen, many of the principal observations extracted from the very popular and reviewed above studies dedicated to CO oxidation, may be adapted for studying the potential application of perovskites in the PROX reaction. In both cases, the key point is the contribution of the structure of defects of such networks. For instance Peña and Fierro [9] showed the comparison of the CO oxidation reaction carried out with O2 or with N2O on BaTiO3 solids. Differences in the activation energy of these reactions near the Curie temperature of the catalyst and a very slow reaction rate in the temperature range from 373 to 473 K were observed, being limited by the desorption of CO2 under steady-state conditions. These features were considered for proposing that the CO oxidation proceeds via surface defects, confirming that the defects into the perovskite structures are crucial for their application in the oxidation of CO.
19 In the same review, in a section devoted to oxidation reactions over perovskites [9], there is an interesting summary of how the CO oxidation proceeds according to a suprafacial process where the band structure near the Fermi level seems to be important in the electronic transfer, being influenced by the temperature and the O2 partial pressure. For LaBO3 perovskites (being B = transition elements from V to Ni), the LaCoO3 proved to be one of the most active and the LaCrO3 among the least active for the CO oxidation. In this sense Tascon et al. [39] have proposed a mechanism for the CO oxidation on LaCoO3. Oxygen is adsorbed as molecular O2- on Co2+ and then is dissociated in atomic O-. On the other hand, CO adsorbs on surface oxide ions, producing labile species that interacts with adsorbed atomic oxygen for producing carbonate species which is then decomposed to afford adsorbed CO2 and oxygen. In other study about nonstoichiometric LaCuO3-δ (δ = 0.05-0.45) perovskites, it was highlighted how the concentration of oxygen vacancies can be gradually changed by controlled annealing at higher temperatures and oxygen pressures. Additionally, it was observed that catalytic activity in CO oxidation is largely controlled by the number of oxygen vacancies present in the crystal structure as has been confirmed in other works [81, 82]. It means that the ability for controlling the kind and concentration of defects into the structure of the perovskite oxides results relevant for the performance of such materials in oxidation processes. Modulation of the defective structure in perovskites may be carried out through the doping with different cations such in the case of doped Ln1-xSrxNiO3 (Ln = Pr, Sm, Eu) reported by Falcón et al. [83] . The catalytic activity evaluation of the different materials demonstrated that the doped solids were considerably more active that the undoped ones, being especially active those solids doped with Pr. Considering many possible applications of perovskites where the defects in the structure are important, not only the creation but also the mobility of defects is relevant. This last subject has motivated studies on examining principally the oxygen mobility [84], because the application of perovskites as ion conductors has been approached in several fields [9, 81]. In the case of the preferential oxidation of CO, the oxygen mobility results determinant for the activation of the CO molecules and their transformation into CO2. Uberuaga et al. [84] studied the migration mechanisms of
20 interstitials and vacancies in perovskites with different chemical compositions (SrTiO3, SrTiO3, BaTiO3, LaAlO3), varying the potential to simulate long time dynamics. They found that the migration mechanisms for the various interstitial and vacancy species are very similar regardless of the potential used of the chemistry of the perovskite, though the energy barriers associated to those mechanism are sensitive to both parameters. Additionally, oxygen and A cation interstitials (in a ABO3 structure) diffuse in a complex manner, exhibiting one- or two-dimensional diffusion mechanisms that are detected in the long-time simulations. The demonstration of the high oxygen mobility in these materials may agree with the required ability of a PROX catalyst of providing oxygen species from the structure where the concentration of O2 in the gas mixture of reaction is deficient. On the other hand, the high ionic mobility in perovskites may also contribute to the enhancement of the mass transport phenomena during the catalytic process, which is a relevant aspect for the scaling up of the PROX reaction and its linkage to a fuel processor. The specific applying of perovskites in the PROX reaction has been proposed in some works such as that published by Maluf et al. [85] where LaNiO3, La0.95Ce0.05NiO3 and La0.90Ce0.10NiO3 have been synthesized by co-precipitation of the adequate amounts of La, Ce and Ni nitrates. The TPR results showed that reduction of these mixed oxides proceeds in three steps and, in the case of the solids with cerium, the reduction of Ni3+ to Ni2+ species occurred at lower temperatures by the enhancement of the oxygen mobility. Concerning the catalytic activity, none of the samples presented CO conversion at temperatures below 150 ºC but the solids doped with Ce presented a better catalytic activity. However, comparing between these samples, the excess of Ce in the La0.90Ce0.10NiO3 reduced dramatically the interaction Ce–Ni by the promoted increment of defects, allowing the formation of segregated phases and reducing the ionic mobility. In this sense, an optimal concentration of defects for enhancing the CO oxidation abilities of the analyzed perovskites is suggested. Gosavi et al. [86] studied the PROX reaction over platinum supported on lanthanum ferrite-ceria (Pt/LaFeO3-CeO2) catalysts, modifying the loading of Pt (0.5, 1.0, 2.0 and 5.0 wt.%). The supports were synthesized using chitosan complex and, an additional LaFeO3 system was prepared by the sol-gel method in order to evaluate differences in the textural properties promoted by the synthesis procedures and their
21 influence in the catalytic activity. The using of chitosan complex allowed an improved crystallinity and homogeneity of the material, together with a higher porosity and open morphology. These properties resulted in a strong Pt-support interaction, producing a high catalytic performance of the materials, combining high CO conversion and selectivity to CO oxidation. In other work [87], the same authors have proposed a study where various oxides including perovskites with a kind of oxygen defective structure (CeO2, CuLa2-CeO2, La2CuO4), widely employed as superconductor, were used as supports for supporting 0.1 Pt wt.%. The obtained materials were tested in the cited catalytic reaction and the authors have observed that the La2CuO4 solid presented a considerable CO conversion. Whereas, 0.1 wt.% Pt/CuLaO2-CeO2 presented not only the highest CO conversion levels but also high selectivity. Although there was not a deep analysis on this manuscript and the applied characterization techniques were scarce, the highest catalytic performance of the 0.1 wt.% Pt/CuLaO2-CeO2 was attributed to the enhancement of the WGS reaction at the interface of Pt-metal oxide besides the relatively higher oxidation activity of the metal oxides. Surely, the presence of defects in the structure promoted by the mixture CuLaO2-CeO2 did allow the promotion of dispersion of Pt and the activation of the CO molecules due to the highly mobile oxygen species. In other work presented by Magalhães et al. [88], La1-xCexCoO3 (x = 0, 0.05 and 0.1) perovskite-type oxides were prepared, characterized and evaluated in the PROX reaction. For the synthesis of the materials, a citrate synthesis methodology was applied, favoring the formation of perovskites with rhombohedral structure. TPR studies demonstrated that the inclusion of Ce inhibited the formation of intermediates during the reduction process and generated modifications in the perovskite lattice. All the studied materials presented a similar catalytic performance where the maximum CO conversion (near to 100 %) has been achieved around 200 ºC. Higher temperatures enhanced the hydrogen consumption by the probable side reactions (R-WGS and methanation). The LaCoO3 and La0.95Ce0.05CoO3 solids exhibited a good stability during 48 h of continuous operation. Moreover, the influence of H2O and CO2 was a relevant aspect also considered by the authors, since these components are the main products of the reaction and it is important to verify their influence over the catalytic performance of the studied materials. For such analysis, the LaCoO3 catalyst was tested under constant temperature (180 ºC) and space velocity (40,000 cm3gcat-1h-1). Initially the solid
22 was submitted to a mixture of reaction A (A = 1 Vol.% CO + 1 Vol.% O2 + 60 Vol.% H2 + balance He) during 2 h. Then, the inclusion of CO2 and/or H2O was analyzed with the mixtures of reaction B (A + 4 Vol.% CO2), C (A + 3 Vol.% H2O) and D (A + 4 Vol.% CO2 + 3 Vol.% H2O) and the results are presented in Figure 5. Figure 5. CO conversion for LaCoO3 catalyst at 180 ºC under distinct inlet flows. (A = 1 vol.% CO, 1 vol.% O2, 60 vol.% H2 + balance He ; B = A + 4 vol.% CO2; C = A + 3 vol.% H2O; D = A + 4 vol.% CO2 + 3 vol.% H2O). (Reprinted from Magalhães et al. [88], with permission from Elsevier) Their results demonstrated that the presence of both components in the mixture of reaction (which is more close to realistic conditions in a catalytic reformer) has a negative influence in the CO conversion. In the case of CO2, this may be competing for being adsorbed over the active sites with the CO molecules, delaying the CO oxidation reaction. As for the effect of water, this molecule may be physisorbed over the surface of the catalyst establishing a physical blocking of the active sites. Beside the negative effect of CO2 and H2O over the catalytic activity, this may be restored by allowing desorption of the carbonaceous species and water molecules over the surface of the catalysts. Therefore the deactivation process was not due to a structural modification of the perovskite, pointing out the high stability of such materials for the PROX reaction. Chagas et al. [89] also worked with the LaCoO3 perovskite for preparing catalysts for the PROX reaction. The perovskite structure was obtained by the Pechini’s method that implies the polyesterification between citric acid and ethylene glycol, employing La(NO3)3 and Co(NO3)2. Subsequently the obtained material was physically mixed with pretreated -Al2O3 in different proportions (10, 20 and 40 wt.% in
23 perovskite) and finally calcined at 500 ºC for 24 hours. Although the synthesis of the LaCoO3 was successfully achieved, the deposition over the alumina did not result in a highly disperse perovskite phase. In any case, the use of this method did not cause structural changes in the active phase after supporting and heat-treatment steps. The bulk LaCoO3 and the 40 wt.% LaCoO3/Al2O3 sample presented the highest catalytic performances. In the case of the deposited system, although a high dispersion was not achieved, the observed enhancement of the catalytic activity may indicate a large exposition of available area of perovskite for the reaction. 4. Concluding remarks The good catalytic activity of perovskite-type oxides in the CO oxidation reaction is well-known for more than 40 years. During this period of time, a large number of researchers have centered their attention in the study and comprehension of the main factors governing such catalytic performances. Most of the works agree in the key role played by the structure of defects of the perovskite arrangement, which can be tailored adjusting the composition of the solid, mainly by substituting (total or partially) the A and B cation by other ones with the same or different oxidation state. The generation of such cationic or anionic defects alters (normally improving), the electronic, redox, ionic transport and surface properties of the material, and it is generally considered as decisive in the catalytic activity shown by the solid. The high CO oxidation activity of bulk perovskites can be even increased if they are used as supports of any other active metal, particularly noble metal ones. In this case, the settlement of the noble metal on the surface or inside the perovskite structure, as well as the nature of the A and B cations, is determinant. In the latest years, the increasing interest in developing catalyst able to abate CO at low temperature from hydrogen streams for feeding fuel cells, besides the recognized capabilities of perovskites in CO oxidation, and their encouraging and promising characteristics and properties briefly reported above, has motivated the renewed attention in such solids and in their possible application in the H2 clean-up processes, such as WGS and PROX ones.
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