Limin
Chen
*ab,
Yunfeng
Bao
a,
Yuhai
Sun
a,
Ding
Ma
bc,
Daiqi
Ye
a and
Bichun
Huang
a
aGuangdong Provincial Key Laboratory of Atmospheric Environment and Pollution Control, School of Environment and Energy, South China University of Technology, Guangzhou 510006, China. E-mail: liminchen@scut.edu.cn; Tel: +86 20 39380516
bState Key Laboratory of Catalysis, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian 116023, China
cCollege of Chemistry and Molecular Engineering, Peking University, Beijing 100871, China
First published on 21st September 2015
A variety of PtFeNi catalysts supported on carbon materials have been prepared and tested for CO preferential oxidation (PROX) in excess hydrogen. 100% O2 and CO conversions have been achieved over carbon black (CB) and carbon nanotube (CNT) supported PtFeNi catalysts at room temperature in a feed gas containing 1% CO, 0.5% O2 (volume ratio) and H2 balance gas. N2 adsorption, temperature-programmed desorption (TPD) and transmission electron microscopy (TEM) studies indicate that the carbon textural properties and surface chemistry determine the catalyst particle size distribution and mean size; but the mean particle size does not have a great influence on the catalytic performance within the investigated particle size range. X-ray diffraction (XRD), resistance measurements and the designed catalytic reaction results reveal the ability of graphitic carbon to capture and shuttle electrons from the noble metal to spatially different sites in the FeNi species through the π–π network, enables the indirect interactions between Pt and the FeNi species, leading to a strengthened synergistic effect, enhancing the CO oxidation activity at room temperature, increasing the Pt utilization efficiency, and apparently decreasing the Pt loading level.
Among the various catalysts, Pt-based catalysts especially Fe,5–8,20,21 Co,9–14 Ni,14–19,21 Cu,11,22 and Ag23etc. promoted Pt catalysts are the most promising candidates. However, it is extremely difficult to realize the total conversion of CO at ambient temperatures with reasonable costs, which is particularly important for fuel cell applications in transportation.10,13,17,20 To the best of our knowledge, among all the supported Pt catalysts reported in the literature, there are only a few supported Pt catalysts that can accomplish the total conversion of CO at room temperature or even lower,4,5,21 mainly including our PtFe/SiO25 and later developed PtFeNi/CNT21 catalysts.
In order to find effective, low-cost and highly robust Pt-based catalysts, besides the promotion effects of promoters, the effects of various supports on the catalytic performance have been extensively investigated in the promoted catalytic system, including CeO2,11 TiO2,12,14 SiO2,4,5,14 Al2O3,8,11,22 zeolites10 and carbon materials6,9,13–21etc. The results indicated that some supports could help to distribute the active component uniformly,17 and some could interact with the active component24 or influence the chemical state of the active component.12 Especially, Petkov et al. reported the role of support–nanoalloy (PtCoNi) interactions on CO oxidation.14 Their investigation indicated that by controlled thermo-chemical treatment, oxygen activation sites on TiO2 supported nanoalloys could be provided both by the second/third metal sites in the nanoalloy (Type-I sites) and by the anionic oxygen deficiency sites located at the nanoalloy-support perimeter zone (Type-II sites). However, only Type-I sites can be obtained for nanoalloys on carbon supports; neither can be generated on SiO2 supported nanoalloys, resulting in the lowest activity for the silica-supported nanoalloys.
Petkov's research is based on the assumption that the promotion effects of base transition metals originates from Pt-nanoalloys. However, our extensive investigation demonstrated that the coordinatively unsaturated transition metal cations confined in nanosized Pt matrices were the main oxygen-activation sites.5–7,9,21 Therefore, Petkov's discovery could not explain the extremely high activity of SiO2 and carbon materials supported PtM (M = Fe, Ni, Co) catalysts for CO PROX and CO oxidation.5–7,9,13,21 Our previous research indicates that a 3 wt% PtFeNi/CNTs catalyst is extremely highly active, and can almost totally remove CO in the gas composition of 1 vol% CO, 0.5 vol% O2 and H2 balance even at 6 °C.21 Compared with other highly active catalysts,5,6,9,13 this catalyst consists of an evidently lower Pt loading level, operating with stoichiometric O2, a much higher concentration of H2 and nearly the same gas hourly space velocity. Our further investigation indicates that in situ formed coordinatively unsaturated FeOx and/or NiOx species confined in Pt matrices are active species and the over oxidation of Fe and Pt species seriously deactivates the catalysts.21 These discoveries are similar to those found with our previously reported PtFe/SiO2 catalysts;5 then, what leads to the extremely high activity of PtFeNi/CNTs even with apparently lower Pt loadings? Is it due to the unique properties of CNTs or the general properties of carbon?
Recently, the ability of carbon nanotubes and graphene-based systems to capture and shuttle electrons through the π–π network has been confirmed through spectroscopic studies.25,26 This feature enables the incorporation of a semiconductor and Pt nanoparticles into a single graphene or reduced graphene oxide sheet, and the resulting multifunctional photocatalyst has been demonstrated for use in photocatalytic H2 production.27,28 This photocatalyst can carry out selective catalytic processes at separate sites and tune the selectivity and efficiency of photo-catalytic reduction and oxidation processes, independently. As far as our highly active PtFeNi/CNTs catalyst is concerned, do CNTs possess the ability to capture electrons and shuttle them, and will this ability contribute to the high catalytic activity or not?
In order to answer the above questions and reveal the origin of the extremely high activity of the PtFeNi/CNTs catalyst compared with PtFe/SiO2 and other catalysts, four types of carbon: CNTs, carbon black (CB) with high graphitization, oxidized carbon black (CB-o), and activated carbon (AC) with less graphitization, were used to prepare PtFeNi catalysts and the effects of their catalytic properties on CO PROX were tested. CB can be utilized to exclude the unique properties of CNTs, for instance, confinement effects; CB-o can be used to investigate the negative effects of carbon surface oxidation on the ability of carbon to capture electrons and shuttle them; AC can facilitate the deliberation of the roles of the graphitization degree and the well-developed pore structure on the catalytic performance. Therefore, the effect of the properties on the catalytic performance were investigated through N2 adsorption, TPD, TEM, XRD and resistance measurements. The discovery from this research will further direct us to design and prepare more effective, economical and robust catalysts for CO PROX in H2 rich streams.
Transmission electron microscopy (TEM, TECNAI Spirit) was used to study the size of the metal particles. XRD measurements were carried out on a Rigaku D/Max 2500 diffractometer with a Cu Kα monochromatized radiation source at 40 kV and 250 mA. The sheet resistivities were measured by a conventional SZ-82 four-probe instrument (Suzhou Tel. Apparatus Co., China).
Fig. 2 Variation in the O2 conversion (A), CO conversion (B), and selectivity (C) at 23 °C over different carbon supported Fe and Ni promoted Pt catalysts as a function of the reaction time. |
These results indicate that the addition of Fe and Ni can dramatically enhance the catalytic activity of Pt catalysts; additionally, the catalysts can be deactivated to some extent, which has been extensively investigated in our previous publications.5,21 In addition, carbon supports also play important roles in the catalytic performance. On one hand the same PtFeNi catalysts with different carbon supports exhibited different catalytic performances; on the other hand, Pt and PtFeNi catalysts with the same carbon supports gave different catalytic activity trends. For example, the Pt/AC catalyst presented a significantly higher activity (O2 conversion at the same temperature) than Pt/CB-o; on the contrary, the PtFeNi/AC catalyst showed a significantly lower activity (O2 conversion at 23 °C) than PtFeNi/CB-o. Furthermore, it is interesting that all PtFeNi catalysts exhibit relatively stable selectivities although there is some loss in O2 and CO reactivity. In order to elucidate the effects of the carbon supports on the catalytic performance, the catalysts have been investigated by a number of characterization methods (vide infra).
Temperature-programmed desorption (TPD) in an inert gas (He, Ar, N2) is effective in determining the different oxygen-containing groups of carbon materials.29–34 The TPD curves of CO and CO2 from different carbon supports are shown in the ESI† (Fig. S2) and the corresponding integration areas of the CO and CO2 desorption from TPD are listed in Table 1. It is clear that AC has many more acidic oxygen containing functional groups, CB-o possesses a moderate amount of oxygen containing functional groups, CNTs hold fewer oxygen containing functional groups compared with CB-o and AC, and CB hardly bears any oxygen containing functional groups.
The graphitization degree of carbon materials can be reflected using XRD characterization, as shown in Fig. 5. The diffraction peaks at 25.78, 42.88, 53.58 and 78.18° are characteristic of graphitic carbon (JCPDS 656212). The strong and sharp diffraction peaks for the CNTs verify the high graphitization degree of the CNT sample, which is essentially composed of coaxial graphitic cylinders. CB and CB-o show similar but slightly broadened diffraction peaks with a slightly lower intensity compared to that of the CNTs. In comparison, the diffraction peaks of AC are broadened obviously (Fig. 5d), indicating an evidently poorly crystallized graphitic structure. Generally, the high graphitization degree means that there is a complete π–π network, indicating the free movement of delocalized π-electrons on the carbon surface, i.e. the high electrical conductivity of the carbon materials.35 As far as CB-o is concerned, it displays similar diffraction features to CB; however, it bears more surface functional groups, suppressing the movement of π-electrons, resulting in a lower electrical conductivity. Therefore, the conductivity of the carbon materials was measured according to the resistivity measurement, as shown in Fig. 6. The resistivities of CNTs, CB, CB-o and AC are 0.04, 0.45, 1.35 and 141.80 Ω cm, respectively; which implies that the electron conductivity decreases in the order: CNTs > CB > CB-o > AC.
Fig. 6 The resistivities of the supports and the catalytic activities of the Fe and Ni promoted Pt catalysts at 23 °C as a function of the different carbon supports. |
As mentioned in the Introduction section, carbon with a graphitic structure can capture and shuttle electrons to different sites through π–π networks. Furthermore, recent spectroscopic studies have proved the ability of graphene oxide to accept electrons from excited semiconductor nanoparticles and then reduce Ag+ at another site spatially different from that of the semiconductor nanoparticles.25 Based on this observation, a Pt-loaded graphene-Sr2Ta2O7−xNx multifunctional photocatalyst with selective catalytic processes at separate sites has been successfully demonstrated.27 Our previous research demonstrated that coordinatively unsaturated FeOx and/or NiOx confined in nanosized Pt matrices are active species for the PROX of CO and that there are interactions between Pt and the FeOx/NiOy species.5–7,21 All investigations suggest that the ability of graphitic carbon to capture electrons and shuttle them to spatially different sites through π–π networks may tune the interactions between spatially separate Pt and FeOx/NiOy species, i.e. indirect interactions between Pt and the FeOx/NiOy species. This speculation means that the higher the conductivity of the carbon materials, the stronger the indirect interaction is. Furthermore, this indirect interaction between Pt and the FeOx/NiOy species may weaken the CO adsorption on Pt and facilitate oxygen adsorption, enhancing the CO oxidation activity. On the other hand, this indirect interaction may also enable optimum CO adsorption and O2 adsorption on Pt and the FeOx/NiOy species, respectively; then the CO oxidation reaction can proceed through a chemical reaction–diffusion wave, as proposed in the previous publications.23,36 There are also other possibilities, such as metal modified carbon catalyzed CO PROX reactions, extensively studied in electro-catalysis recently.37–40 Either way will enhance the Pt utilization efficiency, leading to better or similar catalytic performances with relatively low Pt loadings. This concept is illustrated in Fig. 7 in detail.
In order to verify the above concept, the relationship between the conductivity and the catalytic performance was investigated, as shown in Fig. 6. It is interesting that the electron conductivity of the carbon materials agrees very well with the catalytic activities of the corresponding catalysts, which can be seen from the plots of the CO and O2 conversions. The PtFeNi catalysts supported on the highly electronically conductive supports, such as CNTs, CB and CB-o, exhibit high CO conversions; however, when supported on the carbon materials with low electron conductivities, such as AC, they display low catalytic activities. Besides the high CO oxidation activity of the PtFeNi catalysts, the deactivation rate of the different carbon supported catalysts follows the order AC > CB-o > CB > CNTs. The results indicated that both the CO oxidation activity and stability agree well with the electronic conductivity of the carbon support. This implies that strong indirect interactions may lead to good catalytic performance. This observation confirms that the graphitic carbon strengthens the synergetic effect between Pt and FeNi, leading to high catalytic performance with low Pt loading levels.
It is well known that X-ray photoelectron spectroscopy (XPS) is a good way to characterize the interactions between metals and supports and/or metals and promoters. Therefore, XPS characterization was conducted. However, there is a very low signal for Fe 2p and Ni 2p due to their low loading level. Generally, different catalyst preparation methods will also influence the metal–support interactions; sometimes even changing the structure of the active phase. Thus, different catalyst preparation methods have been designed to adjust the graphitic carbon induced indirect interactions to investigate their effects on the catalytic performance.
Fig. 8 compares the catalytic performance of CB supported FeNi promoted Pt catalysts with different preparation methods. The FeNi(H500)Pt catalyst exhibits an apparently higher catalytic activity and stability compared with the FeNiPt and PtFeNi catalysts. Before being impregnated with the platinum precursor, FeNi/CB was pre-reduced with H2 which will produce elemental iron/nickel and obtain stronger metal–carbon interactions simultaneously. When impregnated with the platinum precursor, the nucleation is prone to occur around the FeNi particles, which is helpful to create active species (it shortens the distance between the Pt and FeNi nanoparticles). Therefore, this preparation method contributes to stronger indirect interactions, resulting in better catalytic performance. This example verifies that the graphitic carbon induced indirect interactions between Pt and the FeNi species play an important role in the synergistic effects. And the catalytic performance difference between CNTs and CB supported PtFeNi may be due to the unique properties of CNTs.
Fig. 8 Variation in the O2 conversion (A), CO conversion (B), and selectivity (C) at 23 °C over CB supported Fe and Ni promoted Pt catalysts as a function of the reaction time. |
In order to further prove the important effects of the graphitic carbon induced indirect interactions on the synergistic effects, highly conductive flake graphite (FG) supported Pt and FeNi catalysts were physically mixed by grinding to prepare PtFeNi/FG catalysts and their catalytic properties for CO PROX were evaluated as shown in the ESI† (Fig. S3). This series of catalysts can effectively exclude the interfacial effects of Pt–FeNi and the alloying effects of PtFeNi on the performances; and the promotion effects should come from the graphitic carbon induced indirect interactions if they exist. It is very interesting that both the CO and O2 conversions are enhanced sharply compared with those of the Pt/FG and FeNi/FG catalysts, as shown in Fig. S3.† This is a good example to confirm the significant roles of the graphitic carbon induced indirect interactions in the synergistic effects.
Thus, carbon materials with graphitic structures can capture electrons and shuttle them to spatially different sites, which induces indirect interactions between Pt and the FeNi species, consolidating the synergistic effects, leading to high catalytic activities of PtFeNi/CNTs catalysts with much lower Pt loadings. The roles of the graphitic carbon induced indirect interactions between Pt and the transition metal species on the thermal catalytic processes have rarely been recognized, although their roles in electrochemical activity and durability of the fuel cell catalytic layers are well understood. This discovery may pave the way to further reduce the loading level of the noble metal and search for more optimal and economical catalysts for the CO PROX reaction and other thermal catalytic processes.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c5cy01091h |
This journal is © The Royal Society of Chemistry 2016 |