Xiaolong 
            Liu
          
        
       *a, 
      
        
          
            Junlin 
            Zeng
          
        
      a, 
      
        
          
            Wenbo 
            Shi
          
        
      ab, 
      
        
          
            Jian 
            Wang
          
        
      a, 
      
        
          
            Tingyu 
            Zhu
          
        
      *ac and 
      
        
          
            Yunfa 
            Chen
          
        
      a
*a, 
      
        
          
            Junlin 
            Zeng
          
        
      a, 
      
        
          
            Wenbo 
            Shi
          
        
      ab, 
      
        
          
            Jian 
            Wang
          
        
      a, 
      
        
          
            Tingyu 
            Zhu
          
        
      *ac and 
      
        
          
            Yunfa 
            Chen
          
        
      a
      
aBeijing Engineering Research Center of Process Pollution Control, National Engineering Laboratory for Hydrometallurgical Cleaner Production Technology, Institute of Process Engineering, Chinese Academy of Sciences, Beijing 100190, China. E-mail: liuxl@ipe.ac.cn; tyzhu@ipe.ac.cn;  Fax: +86 010 82544821;   Tel: +86 010 82544821
      
bState Key Laboratory of Heavy Oil Processing, China University of Petroleum (Beijing), Beijing 102249, China
      
cCenter for Excellence in Regional Atmospheric Environment, Institute of Urban Environment, Chinese Academy of Sciences, Xiamen 361021, China
    
First published on 28th November 2016
In this work, ruthenium-based bimetallic catalysts of the formula Ru–5M/TiO2 (M = Mn, Co, Ce, Cu, Fe) were prepared and evaluated in benzene oxidation, and Ru–5Co/TiO2 exhibited the lowest complete oxidation temperature (220 °C), demonstrating Co3O4 as the best dopant. The influence of the Ru and Co contents on the catalytic activity was also studied, and 1 wt% Ru and 5 wt% Co3O4 were confirmed. Water vapor showed an inhibition effect on benzene oxidation at 210 °C, whereas the catalytic efficiency was barely influenced at a higher temperature (230 °C). STEM analyses revealed that Ru–Co bimetallic species showed similar distributions on the catalytic surface. Based on the correlation of the catalytic results with various characterization techniques, the synergistic effect between Ru and Co was well demonstrated, and a four-step transformation in the oxidation process was concluded. Besides, systematic in situ FTIR studies for benzene oxidation over Ru/TiO2, Co/TiO2, and Ru–5Co/TiO2 were conducted and compared, and many organic intermediates were observed in the in situ FTIR spectra. Accordingly, the reaction mechanism for benzene oxidation over the Ru–Co bimetallic catalyst was proposed.
Bimetallic catalysts commonly show higher catalytic activity, selectivity, and anti-poisoning ability than monometallic materials,22–26 due to the ensemble effect, electronic effect, and the generation of new active sites with the doping of a second metal species. The promotion of performance is generally defined as a bimetallic synergistic effect.27,28 O'Shea et al. prepared Pd–Mn materials and employed these catalysts in methane oxidation, and a Pd–Mn synergistic effect was observed.29 Jodaei et al. reported Ag–M (M = Fe, Co, Mn)-ZSM-5 catalyzed ethyl acetate oxidation, and Ag–Fe-ZSM-5 showed the highest catalytic activity.30 These results revealed that selecting appropriate bimetallic species might be a vital factor for accomplishing the bimetallic synergistic effect.
Ruthenium catalysts have attracted increasing importance in CO oxidation,31 the Deacon process,32 and catalytic oxidation of VOCs.33,34 However, ruthenium-catalyzed VOC oxidations are surprisingly far less investigated than other noble metals. Recently, complete oxidation of ethyl acetate,35 propane,36,37 toluene,38 chlorobenzene,39,40 and trichloroethylene41 has been well established. Nonetheless, it has to be also pointed out that Ru materials still showed slightly lower activity than Pt and Pd catalysts for some common VOCs, such as toluene and benzene, which belong to an important class of VOCs.17,38,42 Doping a transition metal oxide with high oxygen mobility into a Ru catalyst may be an effective strategy to increase its catalytic activity.
Cobalt oxide has been regarded as an attractive material in VOC purification due to its oxygen mobility in Co3+/Co2+ redox, which has been proven to be an important factor in the oxidation process.43 For VOC oxidation, it is generally concluded that its great oxygen transfer ability is attributed to the weak Co–O within the spinel Co3O4 structure.44 Co3O4 has been tested as an active species,19 dopant,22,45 or support.46–48 However, efforts should be continuously devoted to further improve its applicability.
Hence, using Co3O4 as the dopant for noble metals, such as Ru, is very conducive to optimizing the catalytic performance of the present Ru-based catalysts. To the best of our knowledge, complete oxidation of VOCs over a Ru–Co bimetallic catalyst has not been reported. Herein, a series of Ru–Co/TiO2 samples were prepared and evaluated in the catalytic oxidation of benzene. Their catalytic activities were well correlated with the physicochemical properties. Besides, in situ FTIR studies were also conducted, and the reaction mechanism was accordingly proposed.
Ru–(y)Co/TiO2 (y = 1, 3, 5, 10) and (y)Ru–5Co/TiO2 (y = 0.05, 0.1, 0.2, 0.5, 1.0, 2.0) were prepared using the same method by adjusting the contents of Ru and Co3O4. 5Co–Ru/TiO2 was synthesized with the sequence of Ru first and Co3O4 second under the same conditions. (Ru–5Co)/TiO2 was obtained using a co-impregnation method under the same conditions with just one impregnation step.
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 mL g−1 h−1. The reactants and products were analyzed on-line with a gas chromatograph (GC 2010 Plus, Shimadzu) equipped with a flame ionization detector (FID). CO2 and CO at the outlet were detected using another FID with a methanizer (MTH, Shimadzu) furnace. The conversion of benzene was calculated using eqn (1).
000 mL g−1 h−1. The reactants and products were analyzed on-line with a gas chromatograph (GC 2010 Plus, Shimadzu) equipped with a flame ionization detector (FID). CO2 and CO at the outlet were detected using another FID with a methanizer (MTH, Shimadzu) furnace. The conversion of benzene was calculated using eqn (1).|  | (1) | 
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 mL g−1 h−1 within the range 150–300 °C. As shown in Fig. 1A, the catalytic activity increased in the sequence of Ru–5Cu/TiO2, Ru–5Mn/TiO2, Ru–5Fe/TiO2, Ru/TiO2, Ru–5Ce/TiO2, and Ru–5Co/TiO2 with a 90% conversion temperature (T90) of 266 °C, 233 °C, 232 °C, 229 °C, 226 °C, and 215 °C, respectively. It can be seen that Ru–5Co/TiO2 and Ru–5Ce/TiO2 showed higher catalytic efficiencies than Ru/TiO2, whereas other dopants showed a negative effect. It is noteworthy that Ru–5Co/TiO2 gave the lowest complete oxidation temperature of 220 °C, which is comparable to a reported Pd catalyst,17 revealing that Co3O4 was the most appropriate dopant in benzene oxidation. Its higher catalytic activity was tentatively ascribed to the oxygen mobility in the Co3+/Co2+ redox, which might play an important role in the bimetallic catalyzed oxidation. Hence, the Ru–Co bimetallic catalytic system was selected and employed in the following research.
000 mL g−1 h−1 within the range 150–300 °C. As shown in Fig. 1A, the catalytic activity increased in the sequence of Ru–5Cu/TiO2, Ru–5Mn/TiO2, Ru–5Fe/TiO2, Ru/TiO2, Ru–5Ce/TiO2, and Ru–5Co/TiO2 with a 90% conversion temperature (T90) of 266 °C, 233 °C, 232 °C, 229 °C, 226 °C, and 215 °C, respectively. It can be seen that Ru–5Co/TiO2 and Ru–5Ce/TiO2 showed higher catalytic efficiencies than Ru/TiO2, whereas other dopants showed a negative effect. It is noteworthy that Ru–5Co/TiO2 gave the lowest complete oxidation temperature of 220 °C, which is comparable to a reported Pd catalyst,17 revealing that Co3O4 was the most appropriate dopant in benzene oxidation. Its higher catalytic activity was tentatively ascribed to the oxygen mobility in the Co3+/Co2+ redox, which might play an important role in the bimetallic catalyzed oxidation. Hence, the Ru–Co bimetallic catalytic system was selected and employed in the following research.
        In order to determine the best preparation method, Ru–5Co/TiO2, 5Co–Ru/TiO2, and (Ru–5Co)/TiO2 were prepared and compared in benzene oxidation. As shown in Fig. 1B, Ru–5Co/TiO2 exhibited the highest catalytic activity, and 5Co–Ru/TiO2 and (Ru–5Co)/TiO2 were almost comparable with each other within the full temperature range, giving the same T90 of 227 °C (Table S1†). It can be seen that the impregnation sequence plays an important role in the synthesis of bimetallic catalysts with a synergistic effect.
A series of Ru–Co/TiO2 catalysts with different Ru or Co3O4 contents were then synthesized and employed in benzene oxidation (Fig. 1C and D). For Ru–(y)Co/TiO2 (y = 1, 3, 5, 10), Ru–5Co/TiO2 gave the highest catalytic efficiency. The T90 of Ru–1Co/TiO2, Ru–10Co/TiO2, and Ru–3Co/TiO2 were 220 °C, 225 °C, and 227 °C, respectively (Table S1†). For (y)Ru–5Co/TiO2, the catalytic activity apparently increased with the improvement of the Ru content from 0.05% to 2%, and their T90 were 295 °C, 278 °C, 249 °C, 229 °C, 215 °C, and 210 °C, respectively. However, considering the applicability of Ru catalysts, 1 wt% Ru and 5 wt% Co3O4 were confirmed and employed in the following studies.
The anti-moisture performance of the catalyst is crucial to its applicability in VOC purification for industrial off-gas. Hence, the catalytic oxidation of benzene was carried out in the presence of 1 vol% H2O, and the results are summarized in Fig. 2. When the temperature was 230 °C, introduction of H2O led to a very slight decrease of the conversion, and the catalytic efficiency was recovered with the cut off of H2O. When the temperature was set at 210 °C, benzene conversion was stabilized at around 80%. Addition of H2O led to a sharp decrease of benzene conversion by ca. 40%, revealing that H2O exhibited an inhibition effect on the catalytic oxidation process by occupying the reactive sites on the catalyst surface. When H2O was cut off, at first, the catalyst gave an apparently higher benzene conversion than before possibly due to the unbalanced heat release. Gradually, the catalytic efficiency was balanced.
|  | ||
| Fig. 3 XRD patterns of (A) Ru/TiO2 and Ru–5M/TiO2 (M = Mn, Co, Ce, Cu, Fe), and (B) Ru–(y)Co/TiO2 (y = 1, 3, 5, 10). | ||
TEM and HR-TEM were conducted to observe the morphology of Ru–(y)Co/TiO2 catalysts. As shown in Fig. 4, ruthenium species were not observed. HRTEM images were collected and presented in Fig. 4b, e, h, and k. Interplanar lattice spacings for rutile (110) and anatase (101) were observed for TiO2, and cobalt oxide with clear lattice spacings was not observed. To analyze the Ru and Co species, their corresponding EDX spectra were also collected (Fig. 4c, f, i, and l). The EDX spectra confirmed the presence of Ti, O, Ru, and Co elements. With the increase of Co3O4 loading, the Co intensity strengthened obviously. Additionally, TEM and EDX characterization were also recorded for Ru–5Co/TiO2, 5Co–Ru/TiO2, and (Ru–5Co)/TiO2, respectively, and no obvious difference was observed (Fig. S2†).
The dispersion of the active species is commonly correlated with the activity of the catalyst. For many ruthenium oxide-containing materials, the ruthenium oxide exists as thin layers,32 which were hard to observe in the TEM images due to their low contrast. However, STEM methods are commonly used to explore the element distributions, which might afford the interpretation of the catalytic results. Hence, HAADF-STEM and STEM-EDS mapping images were collected for Ru–5Co/TiO2, which exhibited the highest catalytic activity in benzene oxidation. As shown in Fig. 5, a dark field-scanning mode was employed. The support was clearly observed, whereas the bright spots were not confirmed to be the ruthenium species or caused by overlapping TiO2 particles. Accordingly, STEM-EDS mapping was collected. Fig. 5c–e present the distributions of Ru (green), Co (red), and Ti (yellow), respectively. The superimposition of Ru and Co revealed that Ru and Co exhibited similar distribution behavior (Fig. 5f), which might induce the bimetallic synergistic effect to a great extent, leading to an outstanding catalytic performance. Besides, Fig. 5g shows the superimposition of Ru, Co, and Ti, revealing an inhomogeneous distribution of Ru–Co species on TiO2 (P25), which is consistent with previous reports.41,42
|  | ||
| Fig. 5 Representative HAADF-STEM images (a and b) and STEM-EDS mapping images of (c) Ru, (d) Co, (e) Ti, (f) Ru–Co, and (g) Ru–Co/Ti for the Ru–5Co/TiO2 catalyst. | ||
H2-TPR experiments were conducted to investigate the reducibility of Ru/TiO2, 5Co/TiO2, and Ru–5Co/TiO2. As shown in Fig. 6, the Ru/TiO2 sample gave a single reduction peak at 95 °C, which can be assigned to the reduction of RuO2 to Ru.36 For 5Co/TiO2, two main reduction peaks appeared at 294 °C and 419 °C, corresponding to the reduction of Co3O4 to CoO and CoO to metallic Co, respectively.22 As for the bimetallic catalyst Ru–5Co/TiO2, the reduction peak of RuO2 still remained at 95 °C, whereas the reduction peaks of cobalt oxides appeared at 142 °C and 274 °C, respectively. Obviously, the reducibility of cobalt oxides was enhanced, suggesting a synergistic effect between Ru and Co in Ru–5Co/TiO2. This phenomenon is generally defined as the hydrogen spillover effect, and it is commonly observed in the low-temperature reduction of a transition metal oxide in the presence of a noble metal.28
The XPS spectra for Ru–(y)Co/TiO2 (y = 1, 3, 5, 10), 5Co–Ru/TiO2, and (Ru–5Co)/TiO2 were collected, and the Ru 3d and O 1s spectra are summarized in Fig. 7. The assignments and definitions of Ru peaks were controversial and inconsistent with previous studies.49,50 In this research, the Ru 3d spectra were tentatively deconvoluted into three peaks at 280.2, 281.4, and 282.6 eV, assignable to Rucus (coordinatively unsaturated site), Rucus + Oot (Rucus bonded with on-top O), and Ru4+satellite (satellite peak of Ru4+), respectively.42,51 Rucus has been demonstrated to be a catalytically active site, since the adsorbed O species and organic reactants could be easily transferred onto Rucus due to its unsaturated property.42,51 As illustrated in Fig. 7A and Table S2,† Ru–5Co/TiO2 had the most abundant Rucus, which would greatly facilitate the oxidation process.
As shown in Fig. 7B, O 1s spectra were deconvoluted into two peaks at 529.8 eV and 531.8 eV, assignable to Olatt (lattice oxygen) and Oads (adsorbed oxygen, e.g., O2−, O22−, or O−), respectively.52 It has been generally regarded that the electrophilic Oads species play an important role in the catalytic oxidation of VOCs.53 As summarized in Table S2,† Ru–5Co/TiO2 exhibited the highest Oads/Olatt molar ratio of 0.116. For 5Co–Ru/TiO2 and (Ru–5Co)/TiO2, their Oads/Olatt values were almost equal (0.071), and their catalytic curves were basically overlapped (Fig. 1B). Hence, a four-step transformation in the oxidation process was proposed. Firstly, a Co(III)/Co(II) transformation was initiated, and Oads was released (eqn (2)). Then, Co(II) was oxidized into Co(III) (eqn (3)). Subsequently, Oads and organic reactants (Rorg) were easily transferred onto Rucus due to its unsaturated property, generating Ru–O–Rorg species (eqn (4)). Finally, Ru–O–Rorg species decomposed into CO2 and H2O through a series of complicated steps (eqn (5)).
| Co(III) − O → Co(II) + Oads | (2) | 
| Co(II) + [O] → Co(III) − O | (3) | 
| Rucus + Oads + Rorg → Ru − O − Rorg | (4) | 
| Ru − O − Rorg + [O] → Rucus + CO2 + H2O | (5) | 
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif) O from quinone or other ketone species according to previous research.56 The bands at 1532–1519, 1429, 1313–1303 cm−1 were attributed to maleate species.54,57 The band at 1558 cm−1 was assigned to the COO– stretching vibration of surface acetates, and the band at 1375 cm−1 was attributed to the CH3 stretching vibration of surface acetates.54,57 For Co/TiO2, the broad band at 1537 cm−1 should be attributed to the superposition of the maleate and acetate species. Notably, it was confusing to assign the bands at 1863 and 1451 cm−1 in the spectra of Ru–5Co/TiO2 and Ru/TiO2, since these bands were totally missing for Co/TiO2.
O from quinone or other ketone species according to previous research.56 The bands at 1532–1519, 1429, 1313–1303 cm−1 were attributed to maleate species.54,57 The band at 1558 cm−1 was assigned to the COO– stretching vibration of surface acetates, and the band at 1375 cm−1 was attributed to the CH3 stretching vibration of surface acetates.54,57 For Co/TiO2, the broad band at 1537 cm−1 should be attributed to the superposition of the maleate and acetate species. Notably, it was confusing to assign the bands at 1863 and 1451 cm−1 in the spectra of Ru–5Co/TiO2 and Ru/TiO2, since these bands were totally missing for Co/TiO2.
        To demonstrate the unidentified bands, in situ FTIR experiments for (y)Ru–5Co/TiO2 (y = 0.05, 0.1, 0.2, 0.5, 1.0) were also conducted (Fig. 9). Most bands could be identified as discussed above, and the two main sets of the bands between 1600 and 1400 cm−1 showed a representative variation tendency with the improvement of Ru content. Surprisingly, the band intensity at 1863 cm−1 decreased with the improvement of Ru content. In previous studies, the bands between 1900 and 1750 cm−1 were commonly regarded as stretching vibrations of C![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif) O for anhydride (O
O for anhydride (O![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif) C–O–C
C–O–C![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif) O, 1870 cm−1),58 acyl chloride (O
O, 1870 cm−1),58 acyl chloride (O![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif) CCl, 1842 cm−1),59 or aldehyde species (R–CHO, 1755 cm−1).54 In this research, no chlorine was introduced, and they were not quite consistent with the wavenumbers for aldehyde species. Hence, they should be due to the anhydride species, such as maleic anhydride. As for the decreasing tendency, it was tentatively proposed that most Ru species dispersed as small RuOx clusters at lower loadings (≤0.2 wt%), and the π donor of maleic anhydride could be easily coordinated to Ruδ+ at the corner sites of the small RuOx clusters, whereas the coordination behavior could not be established in the Co/TiO2 system. With more Ru addition, Ru nanoparticles were formed, and most Ru species were present as RuO2, which were inclined to adsorb other organic salt species, leading to the weakening of the band intensity for maleic anhydride. Besides, it was reasonable to assign the band at 1451 cm−1 to the COO– stretching vibration of surface acetates adsorbed on Ru centers.55
CCl, 1842 cm−1),59 or aldehyde species (R–CHO, 1755 cm−1).54 In this research, no chlorine was introduced, and they were not quite consistent with the wavenumbers for aldehyde species. Hence, they should be due to the anhydride species, such as maleic anhydride. As for the decreasing tendency, it was tentatively proposed that most Ru species dispersed as small RuOx clusters at lower loadings (≤0.2 wt%), and the π donor of maleic anhydride could be easily coordinated to Ruδ+ at the corner sites of the small RuOx clusters, whereas the coordination behavior could not be established in the Co/TiO2 system. With more Ru addition, Ru nanoparticles were formed, and most Ru species were present as RuO2, which were inclined to adsorb other organic salt species, leading to the weakening of the band intensity for maleic anhydride. Besides, it was reasonable to assign the band at 1451 cm−1 to the COO– stretching vibration of surface acetates adsorbed on Ru centers.55
In order to confirm the oxidation-initiation step, an in situ FTIR study during the adsorption of benzene/Ar at 240 °C over Ru–5Co/TiO2 was conducted, and the results are summarized in the ESI.† As shown in Fig. S3,† three main broad groups of bands at 1600–1500 cm−1, 1450–1400 cm−1, and 1375–1350 cm−1, were observed. It is noteworthy that the spectra displayed similar band regions to those in Fig. 8A, and the band intensities slowly increased over time. The band intensities were relatively weaker than those of the spectra collected with O2 possibly due to the oxygen deficiency along with the oxygen-consuming process. Hence, it was believed that the oxidation was initiated by the activation of lattice oxygen (eqn (2)) but not from the activation of molecular oxygen.
As shown in Fig. 10, the reaction mechanism was proposed. On the Ru–Co catalyst (A) surface, benzene (B) first reacts with the Ru–Co centers, generating the phenolate species (C). The oxygen-containing group is generally regarded as an electron-donating group and an ortho–para position director. Hence, the phenolate species are easily transformed into o-benzoquinone (D) and p-benzoquinone (E). With the promoting effect of Ru–Co, a ring-opening proceeds under the attack of active oxygen species, and some small organic intermediates are generated, such as maleates (F), acetates (G), and ketones (H). Eventually, the intermediates are oxidized into inorganic products CO2 and H2O, and the Ru–Co catalyst is recovered.
| Footnote | 
| † Electronic supplementary information (ESI) available: Various characterization analyses and evaluation data for the catalysts, and CO2 selectivity of benzene oxidation over Ru–5Co/TiO2. See DOI: 10.1039/c6cy02141g | 
| This journal is © The Royal Society of Chemistry 2017 |