Carlos
Hernandez-Mejia
a,
Edwin S.
Gnanakumar
a,
Alma
Olivos-Suarez
b,
Jorge
Gascon
b,
Heather F.
Greer
c,
Wuzong
Zhou
c,
Gadi
Rothenberg
a and
N.
Raveendran Shiju
*a
aVan't Hoff Institute for Molecular Sciences, University of Amsterdam, P.O. Box 94157, 1090GD Amsterdam, The Netherlands. E-mail: n.r.shiju@uva.nl; Web: http://hims.uva.nl/hcsc
bDelft University of Technology, Catalysis Engineering Section, Julianalaan 136, 2628 BL Delft, The Netherlands
cSchool of Chemistry, University of St Andrews, St Andrews KY16 9ST, UK
First published on 24th August 2015
Effective dispersion of the active species over the support almost always guarantees high catalytic efficiency. To achieve this high dispersion, a favourable interaction of the active species with the support is crucial. We show here that the crystal structure of the titania support determines the interaction and consequently the nature of ruthenium particles deposited on the support. Similar crystal structures of RuO2 and rutile titania result in a good lattice matching and ensure a better interaction during the heating steps of catalyst synthesis. This helps maintain the initial good dispersion of the active species on the support also in the subsequent reduction step, leading to better activity and selectivity. This highlights the importance of understanding the physico-chemical processes during various catalyst preparation steps, because the final catalyst performance often depends on the type of intermediate structures formed during the preparation.
For heterogeneous catalysts, the active species such as the metal is often supported on a high surface area metal oxide. The interaction between metals and oxide supports, so-called metal-support interactions, then becomes important.38 Tauster et al. proposed the concept of strong metal-support interaction (SMSI) in 1978 to describe the drastic changes in the chemisorption properties of Group 8–10 noble metals supported on TiO2.39 Later, SMSI was widely observed in many metal/oxide catalytic systems. Electronic or geometric factors may be responsible for SMSI. The Electronic factors involve charge transfer between the metal and the oxide. As a result, the electronic structure of the metal will be perturbed.
Here we report the catalytic hydrogenation of xylose to xylitol (eqn (1)) using Ru supported on TiO2. We show that the deposition of Ru on TiO2 gives highly efficient catalyst. However, we also show that the efficiency depends significantly on the crystal structure of the support. The key lies in the catalyst preparation steps, wherein the crystal structures of the support and RuO2 determine the mutual interaction and consequently the Ru particle size.
(1) |
Sample | Crystal structure | Preparation | SSAa of calcined catalysts | SSA of reduced catalysts |
---|---|---|---|---|
a SSA: Specific Surface Area (m2 g−1). | ||||
A | Anatase | Hombikat M311 (commercial support) | 86 | 7 |
B | Anatase | Hombikat M311 calcined at 450 °C, 2 h | 47 | 47 |
C | Rutile | Hombikat M311 calcined at 900 °C, 24 h | 2 | 4 |
D | Anatase and rutile | Hombikat M311 calcined at 800 °C, 2 h | 14 | 12 |
For each catalyst, RuCl3 (0.396 mmol) , corresponding to 1 wt% Ru loading, was dissolved in deionized water (50 ml) in a round-bottom flask and heated up to 75 °C using an oil bath. Then titania (4 g) was added into the RuCl3 solution under stirring and left at 75 °C until the water was completely evaporated. The samples were dried at 120 °C for 12 h and were calcined at 400 °C for 3 h. The samples were then reduced at 350 °C for 2 h under H2 atmosphere. The samples were analysed by powder X-ray diffraction (see ESI†).
Examining the substrate conversion and product yield at 120 °C, one sees immediately a striking performance difference between the anatase and rutile supports (Fig. 1). Anatase supported Ru (A) gave a mixture of products, with low xylitol selectivity. Interestingly, Ru supported on rutile titania (catalyst C) gave 100% xylose conversion and up to 98% yield for xylitol in 15 min. Catalyst D showed similar behaviour to C, indicating that the Ru properties are influenced by the rutile part of the support. B was more active and selective than A, though still worse than rutile supported Ru. Note that B is still predominantly anatase, but has a lower surface area compared to A. Thus, the surface area seems not to be critical here. The same trends in performance were observed at 140 °C and 160 °C, albeit that increasing temperature decreased the xylitol yield (see Fig. 1), giving instead more of the diastereomers arabitol and adonitol (Fig. 2).
Fig. 1 Xylitol yield at different temperatures after 3 h reaction. Reaction conditions: 20 bar H2, xylose:Ru ratio 100:1 (w/w), solvent water. |
The kinetic studies at 120 °C (Fig. 3) confirm that C and D are more active and selective than the anatase based catalysts A and B. Xylitol was selectively formed (98%) within 15 minutes over C and D. The selectivity decreased marginally with increasing the reaction time. A does not show a major xylitol yield at any given time. For B, a maximum xylitol yield is observed at 180 min. Full conversion was not achieved with both A and B under these conditions.
A recycling test for C and D was carried out at 120 °C. The reaction mixture after each time was centrifuged and the liquid phase was separated from the catalyst. This liquid phase was analysed and the catalyst was washed with distilled water. Conversions and xylitol yields were constant even after the fourth recycling test, showing the stability of these two catalysts.
In order to explain the activity trends, we characterized the catalysts by several techniques. The XRD patterns (see ESI†) confirmed that A and C are predominantly anatase and rutile respectively. We also calculated the percentage of rutile phase in each catalyst (B, C and D have 1.1%, 99.5% and 34.5% rutile phase, respectively). Note that the most predominant crystallographic plane for anatase is (101) and for rutile is (110).40 These planes were used for calculating the ratio of the phases and for the images shown in Fig. 6. Diffraction peaks corresponding to ruthenium species could not be observed, indicating high dispersion of supported ruthenium. H2 TPR profiles of the calcined catalysts (Fig. 4) show a sharp peak between 180 and 230 °C, which can be assigned to the reduction of RuO2.36,41,42 Hydrogen intake from the catalysts A, B, C and D are 1254, 1438, 739 and 507 μg mol−1 respectively. Anatase-based catalysts have a higher hydrogen consumption compared to rutile catalysts. The second peak on the TPR profile (between 270 and 450 °C) may be ascribed to a partial reduction of the support, inducing the formation of oxygen vacancies or Ti3+ species.43
SEM analysis (ESI†) revealed a uniform dispersion of ruthenium over C after calcination as well as after reduction. In contrast, EDX detected visible metallic agglomerations on the surface of A and B, before and after reduction. We further studied the catalysts by TEM, which provided important information (Fig. 5). The rutile TiO2 particles (Fig. 5b) were of several hundred nanometers in diameter. In contrast, the anatase TiO2 particles (Fig. 5a) were smaller in size. Since the rutile form was obtained by high temperature calcination, formation of the larger titania particles is expected. Importantly, a homogeneous surface covering of Ru particles was observed on rutile surface (C). The typical Ru particle size is between 5–7 nm (see also ESI†). On the contrary, Ru particles were very localised on the anatase surface. These are much bigger (see the dark particle in Fig. 5a) and could easily be detected by EDX (SEM images in ESI†).
Fig. 5 The TEM images of catalysts A (a) and C (b) show the agglomeration of the Ru on the anatase support and the fine dispersion on the rutile support. |
The uniform distribution of Ru nanoparticles with a narrow size distribution over rutile titania (catalysts C and D) suggests a lattice anchoring interaction between Ru and the support. Since RuO2 also has a rutile-type structure, we expect a high degree of lattice matching between RuO2 and the rutile titania support, preventing the agglomeration of Ru particles during the calcination step (Fig. 6, left).44–46 Since there is no such matching with the anatase support, the RuO2 particles are less stable (Fig. 6, right). Thus, the agglomeration of Ru on anatase, as shown by TEM, can explain the lower catalytic performance compared with rutile catalysts. RuO2 nanoparticles are reported to be easily aggregated in oxidative atmosphere due to the volatility of oxidized ruthenium.47 This is the case observed in the RuO2/anatase-TiO2. However, the intimate interaction between RuO2 and rutile-TiO2, as a result of their high degree of lattice matching stabilizes the RuO2 and maintains its high dispersion during calcination and further reduction. The binding nature of RuO2 nanoclusters on rutile TiO2 (110) and anatase TiO2 (101) surfaces was studied by first-principle calculations previously.48 These studies showed that the adsorption energy of RuO2 cluster on rutile is larger than that on anatase due to more interfacial bonds formed between cluster and surface. This further confirms our experimental observations that the rutile support provides highly dispersed Ru with uniform nanosize, leading to high activity and stability in xylose hydrogenation to xylitol. When the support contains both rutile and anatase (D), the Ru is predominantly present on the rutile. We observed such behaviour previously for vanadia supported on Al2O3–MgO. Vanadium species was preferentially attached to Al2O3 at low loadings and to MgO at high loading.49
Fig. 6 Atomic structures of RuO2 on rutile (left) and anatase (right) TiO2 showing the high degree of lattice matching of RuO2 on rutile TiO2 (created by viewerlite software).50 |
We also analysed the catalysts after the reaction by XRD and TEM. The peak at 2θ = 25° was slightly broader for the spent A catalyst. There was no other major change in the XRD patterns before and after the reaction for any of the catalysts (Fig. S2†). TEM images did not show any obvious changes for the spent catalysts (see ESI†). The Ru particles are small and highly dispersed for the spent catalyst C as in the fresh catalysts. This indicates that the structure remains unchanged during the reaction. Indeed, this catalyst retained the same level of activity after multiple recycling tests.
Based on the information from electron microscopy and TPR, we can also infer that large Ru species on anatase TiO2 leads to a higher reducibility of the support. As mentioned before, the peak between 270 and 450 °C in the TPR of anatase-based catalysts may be ascribed to a partial reduction of the support, inducing the formation of oxygen vacancies and Ti3+ species.43 This could happen most likely at the interface between the Ru species and TiO2 support. These species have two main effects. First they alter the charge transfer between the metal and its support leading to changes on the catalyst's performance.51,52 Second, the presence of Ti3+ species interacting with the C–O bond has been related in previous studies34,53 with either a hydrogenolysis pathway where this C–O bond is cleaved or as a Lewis base leading to a retro–aldol reaction (Fig. 7). Thus, the production of glycols by anatase based catalysts can be explained. Moreover, the surface is deficient in oxygen, leading to aldehyde decomposition in favour of oxygen restoration at the lattice, forming different by-products.54,55 All these effects collectively lead to a lower selectivity for the anatase-supported Ru catalysts.
Footnote |
† Electronic supplementary information (ESI) available: XRD, SEM and EDX analysis, characterization of spent samples, detailed product distribution. See DOI: 10.1039/c5cy01005e |
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