Wilbert L.
Vrijburg
a,
Jolanda W. A.
van Helden
a,
Arno J. F.
van Hoof
a,
Heiner
Friedrich
a,
Esther
Groeneveld
b,
Evgeny A.
Pidko‡
*a and
Emiel J. M.
Hensen
*a
aLaboratory of Inorganic Materials and Catalysis, Schuit Institute of Catalysis, Eindhoven University of Technology, P.O. Box 513, 5600 MB Eindhoven, The Netherlands. E-mail: e.a.pidko@tudelft.nl; e.j.m.hensen@tue.nl
bBASF Nederland B.V., De Meern, The Netherlands
First published on 22nd April 2019
Herein we report our efforts to control the size of colloidal Ni nanoparticles (NiNPs) via a seed-mediated approach and to produce supported Ni catalysts that are sinter-resistant. NiNPs are prepared using a mild capping ligand and an external reducing agent at 90 °C to obtain seeds of 3–4 nm, followed by NiNP growth at 220 °C to vary the final size up to 8 nm. These NiNPs were either introduced onto high surface area silica via direct deposition in organic solvents, or encapsulated in mesoporous silica. Encapsulation was determined to be the most promising approach to support the particles. A range of such encapsulated NiNP catalysts were evaluated for CO2 hydrogenation between 200–400 °C: they were comparably active as catalysts reported in the literature, and thermally stable and sinter-resistant for 70 h at 350 °C. Nevertheless, it was found that the Ni phase was redistributed throughout the mesoporous silica network, resulting in Ni catalysts with nearly identical particle size of 4–5 nm, determined by the size of the support pores, after a combination of oxidative and reductive pretreatments. Our approach provides a route to obtain Ni@SiO2 catalysts with a narrow particle size distribution from a range of colloidal NiNP precursors.
The synthesis of supported metal catalysts via colloidal approaches involves two main challenges related to (i) the control of the nanoparticle size and (ii) the controlled deposition of the colloidal nanoparticles onto a support and the removal of the capping ligands to obtain active catalysts. The former challenge has received more attention than the latter, even though the deposition step is crucial to obtain active and stable catalysts.11 Ineffective anchoring of the nanoparticles may lead to significant particle aggregation during high-temperature activation, whereas low temperature treatments may not effectively remove the capping ligands.12,13 Good control over nanoparticle deposition on oxidic supports is particularly important for Ni, which is susceptible to particle sintering. Moreover, despite several studies in recent years aiming to control Ni nanoparticle (NiNP) size, only limited studies have provided synthetic approaches that yielded NiNPs between 1–10 nm, which that were then also deposited on a support to investigate particle sintering after capping agent removal.14
Colloidal nanoparticles are comprised of a metallic core stabilized by long-chain organic ligands (capping/stabilizing agents). Vital to obtaining homogeneously dispersed nanoparticles are homogeneous seed formation (nucleation) of metallic monomers, induced by metal atom (monomer) concentrations surpassing a threshold concentration (supersaturation). Nucleation stops once the monomer concentration drops below the supersaturation concentration, with existing nuclei consuming the remaining monomers in the organic solution (heterogeneous nucleation).15 Synthetic routes to produce NiNPs have usually involved either (i) thermal decomposition of an organometallic precursor to produce and grow the nuclei, or (ii) inducing nucleation using an external reducing agent to reduce Ni2+, either as organometallic complex or salt, to metallic Ni0. In thermal decomposition procedures, Ni is usually reduced by the capping agents present in the solution.16
Thermal decomposition methods for NiNP synthesis have been extensively explored, with Ni(acac)2 often employed as the Ni precursor. Zhang et al. studied the influence of temperature on NiNP size employing only oleylamine (OAm) as both solvent and capping agent.17 Polydispersed particles with a mean diameter of 22 nm were obtained after nucleation and growth at 220 °C, while nucleation was already found to start at 180 °C. A narrow particle size distribution for 20–60 nm NiNPs could be obtained by separating the seed and growth steps in the synthesis. To achieve this, a two-step seed-growth approach was introduced, in which the initial seeds formed at 220 °C could be grown more homogeneously by introducing additional precursor at room temperature and then maintaining the solution at 195 °C. Chen et al. explored a variety of alkylamines as capping agents and reducing agents when preparing NiNPs via thermal decomposition routes, obtaining particles between 10–50 nm.18
In order to improve control over particle sizes, many studies resorted to stronger capping agents. These have primarily involved phosphorous containing ligands,18–23 although sulfur containing agents have also been explored.24,25 Winnischofer et al. screened various ratios of Ni precursors, phosphine, and amine functionalized ligands to control Ni particle sizes between 4.8–16.3 nm.26 Carenco et al. studied the growth mechanism of NiNPs, employing a combination of trioctylphosphine (TOP) and OAm as capping agents.19 Within their work, the authors determined OAm to be an effective reducing agent (and therefore nucleation agent) but a weak capping agent, whereas the phosphine ligand was an efficient capping agent but poor reducing agent for Ni(acac)2. The exclusive use of OAm as both capping and reducing agent led to Ni particles between 50–80 nm under thermal reduction conditions. Their understanding of the nucleation and growth mechanism allowed the authors to tailor particle sizes from 2 to 30 nm by varying the OAm:
TOP ratio, with TOP-only mixtures yielding the smallest particle sizes with a mean diameter of 2 nm.
The key problem with employing phosphorous containing ligands (P-ligands) is that the phosphorous is inevitably incorporated into the Ni lattice, even at temperatures below 220 °C.19,27–29 Calcination at 500 °C was found to be insufficient to remove phosphorous from deposited NiNPs, yielding supported P-containing Ni nanoparticles which were inactive in cyclohexene hydrogenation.30 However, Ni-phosphides were not observed by XRD and the predominant phase in the synthesized NiNPs was metallic Ni. Similar effects have also been observed for Co-based NPs.31 The use of P-containing ligands should therefore be avoided if Ni- and Co-based hydrogenation catalysts are desired.
Thermal decomposition strategies alone are insufficient to achieve particle size control in the absence of P-ligands, particularly if Ni(acac)2 is employed as the Ni precursor. In addition to thermal reduction strategies the use of strong reducing agents such as NaBH4,32,33 hydrazine,34–36 polyols,37 and more recently borane tert-butylamine (BTB) complex have been explored.38,39 Using OAm and oleic acid (OAc) as co-surfactants at 90 °C, Metin and co-workers were able to synthesize monodisperse NiNPs from 3.2 to 5.4 nm by lowering the BTB/Ni ratio from 3/1 to 1/1 respectively.38 Particles smaller than 3 nm were obtained by Li et al. by increasing the temperature at which BTB was injected into the Ni(acac)2 solution from 90 °C to 180 °C.40 However, particle size control to obtain a series of larger particles between 4 to 10 nm was not achieved, which could be desirable when employed in structure–sensitive catalytic reactions such as CO and CO2 hydrogenation.5–8
In addition to accurately controlling the particle size of colloidal NiNPs, their effective and controlled deposition on oxidic supports and subsequent removal of the organic ligands are vital to obtain active and well-defined catalysts. Direct deposition via impregnation methods are facile,1 but Ni is prone to sintering during ligand removal by calcination at elevated temperatures.30 Rinaldi et al. deposited NiNPs on SiO2 and found that high temperature treatments, although effective at reducing the amount of ligands on the NiNP surface, also increased the particle mobility which led to significant sintering from 5 nm to 20 nm after reduction at 500 °C.30 Zacharaki et al. successfully deposited NiNPs on Al2O3 and effectively removed the ligands by thermal treatment with only slight sintering observed after reduction at 400 °C. Complete reduction was not achieved though, and this is necessary for hydrogenation catalysis.14 More robust methods must therefore be developed to support well-defined colloidal nanoparticles and to maintain their dispersion if colloidal routes are to be considered a beneficial approach. To this end, nanoparticle confinement in porous matrices is considered a viable strategy. The stabilization of small (<2 nm) NiNPs through confinement in zeolite micropores has been investigated by Laprune et al.41 and Goodarzi et al.42 Brock and co-workers successfully encapsulated Ni2P colloidal nanoparticles (d = 11 nm) in mesoporous silica to prevent their aggregation after ligand removal and catalyst activation.43 Such strategies have been studied for supporting colloidal Pt and Pd nanoparticles,44–47 as well as phosphorous-free colloidal NiNPs,48–50 although these NiNP studies sought to support and stabilize particles larger than 20 nm. At present, no study has been able to produce well-defined colloidal NiNPs which vary in particle size and maintain their dispersion once supported and thermally activated (i.e. ligand removal and catalyst reduction), and are active in gas phase hydrogenation reactions. Ideally, such an approach would lead to catalysts that are tailored for a specific structure–sensitive reaction.
In this work, we report the preparation of mesoporous silica supported NiNPs prepared via the colloidal approach. By building a comprehensive set of colloidal NiNPs, we are able to isolate important factors controlling growth and nucleation using established colloidal nanoparticle growth theory. A two-step seed-mediated synthetic approach was developed, in which NiNP nucleation was induced with an external reducing agent under mild conditions. Particles were subsequently grown under thermal decomposition conditions (>200 °C) to obtain NiNPs between 3–8 nm using P-free ligands. Next, strategies to support the colloidal NiNPs and remove their ligands were investigated. Encapsulation of NiNPs in mesoporous silica produced active and stable hydrogenation catalysts. Moreover, encapsulation of colloidal NiNPs of different sizes ultimately led to a redistribution of the encapsulated Ni to yield catalysts with identical particle sizes and substantial catalytic activity. This approach demonstrates that colloidal NiNP growth can be effectively controlled using only mild capping agents, but that the support pore size becomes the controlling factor of the final NiNP size in encapsulated Ni@SiO2 hydrogenation catalysts.
To obtain larger particles, the seeds were grown at elevated temperatures. After 1 h of the initial seed formation (as described above), the black solution was heated to 220 °C using a heating mantle. Additional Ni(acac)2 (2–4 mmol) in equimolar OAc (2–4 mmol) was dissolved in octadecene (ODE, 10–20 mL) and was added dropwise to the round-bottomed flask using a Teflon cannula at a rate of ca. 0.5 mL min−1. The particles were kept at 220 °C for an additional 1.5 h, after which the heating mantle was removed. Toluene was added to make a 1:
1 solution with the colloidal NPs. Nanoparticles were precipitated, collected, and washed according to the procedure outlined above.
In order to remove the organic ligands (OAm/OAc) and templating/stabilizing agent (CTAB), Ni@SiO2 was calcined in 20 vol% O2 in N2 mixture (50 mL min−1) at 500 °C (1 °C min−1, 10 h). The oxidized NiO@SiO2 nanoparticles were reduced at 450–550 °C in 10 vol% H2 in He flow (2.5 °C min−1, 6 h).
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Procedure | Initial Ni(acac)2 (mmol) | BTB/Ni | T (°C) | Ni(acac)2 added (mmol) | d (nm) | Fraction Ni0b (%) |
---|---|---|---|---|---|---|
a BTB injection at 90 °C, Ni(acac)2 addition at 220 °C. b Air exposed. Surface fraction determined by XPS. | ||||||
1 | 5 | n/a | 220 | 0 | 53 (± 14) | 47 |
2 | 1 | 5 | 90 | 0 | 4.4 (± 0.5) | 22 |
3a | 1 | 5 | 90, 220 | 2 | 6.3 (± 1.0) | 12 |
4a | 1 | 5 | 90, 220 | 4 | 7.9 (± 1.5) | 39 |
To obtain smaller particles with a narrower size distribution, lower-temperature procedures (90 °C) with an external reducing agent were applied (procedures 2–4, Fig. 1, Table 1).38 Borane tert-butylamine (BTB) was dissolved in OAm and injected into the Ni(acac)2/OAc/OAm solution, turning the mixture black almost instantly (procedure 2). The rapid injection of the external reducing agent leads to a supersaturated solution during which particle nucleation occurs. It is vital that this step is carried out rapidly to achieve homogeneous nucleation and obtain colloidal NPs with a narrow particle size distribution. TEM images confirm that nanoparticles of 4.4 nm were obtained for BTB/Ni = 5 after 1 h growth at 90 °C (Fig. 2b). After precipitating out the NiNPs using a toluene/acetone mixture, the remaining supernatant still appeared slightly green, suggesting that not all the Ni2+ had been reduced.
To obtain larger particles, the nanoparticles were pre-formed at 90 °C and rapidly heated to 220 °C. Additional Ni(acac)2 (2 or 4 mmol) dissolved in OAc (2 or 4 mmol, respectively) and ODE (10 or 20 mmol, respectively) was added dropwise to the colloidal dispersion (procedures 3 and 4 respectively, Fig. 1, Table 1). NiNPs of 6.3 nm and 7.9 nm were obtained in this way by the addition of 2 mmol and 4 mmol Ni(acac)2 to the initial suspension at 220 °C. The Ni2+ concentration and the rate of addition were kept constant during the different procedures.
Structural properties of as-synthesized colloidal NiNPs were studied by XRD (Fig. 3). NiNPs synthesized via the BTB reduction pathway (procedures 2–4) did not exhibit crystalline phases in XRD which we attribute to the small particle size.51,52 Low-intensity contributions between 40–45° are likely from amorphous carbon deposits. In contrast, the XRD pattern of NiNPs synthesized by direct thermal decomposition of Ni(acac)2 showed sharp diffraction peaks at 39.1°, 41.6°, 44.6°, 58.4°, 71.0°, and 78.0° correspond to the (100), (002), (101), (102), (110), and (103) crystal planes of hcp-Ni3C (JCPDS no. 04-0853). The hexagonal lattice constants of a = 2.65 Å and c = 4.35 Å match those reported in literature for hcp-Ni3C.53–55 Colloidal routes providing Ni3C nanoparticles have been reported before during synthesis carried out above 200 °C, with carbon contaminations of the organic surfactants yielding the carbide phase.54–57 However, due to the nearly similar lattice parameters of hcp-Ni3C and metastable hcp-Ni, we cannot only rely on XRD to discern between these two crystal phases.53 The carbide phase was confirmed by XPS measurements of the C 1s region (see ESI†). By etching the NiNP surface with Ar+ ions, a peak positioned at 283.5 eV emerged, which could be attributed to the Ni–C bond.54 This phase is metastable and decomposes into fcc-Ni in reducing atmospheres above 300 °C.58,59 XPS measurements of the C 1s region after Ar+ etching did not reveal a Ni–C phase for these smaller NiNPs (see ESI†).
The nature of the particles was studied further with XPS. XP spectra of colloidal NiNPs after exposure to air were obtained in the Ni 2p3/2 region (Fig. 4). Despite the absence of oxidic Ni phases in XRD, we observed both metallic Ni0 (BE = 852.8 eV) as well as oxidized Ni2+ (main peak BE = 856.0 eV, satellite peak BE = 861.5 eV) on all NiNPs, confirming that the NiNPs readily passivated in air. Larger colloidal NiNPs appeared to be more resistant to passivation as evidenced by a higher Ni0 fraction (Table 1).
Interestingly, our results demonstrate that OAm is an effective capping agent at temperatures at which Ni(acac)2 decomposes (>200 °C).60 This result contrasts earlier findings by Carenco et al., who determined OAm to be a weak capping agent under thermal decomposition conditions, leading to large, polydispersed nanoparticles.19 Based on our data, we speculate that OAm is an adequate capping agent but a poor reducing agent, resulting in an ineffective nucleation and slow growth. The theory of colloidal nanoparticle growth has been reviewed in great detail elsewhere.1,3,15,61,62 In the absence of an external reducing agent, atomic Ni monomer formation is kinetically limited during the temperature ramp to 220 °C. Therefore, once (local) supersaturation is achieved, Ni seeds are formed and the monomer concentration decreases below the threshold concentration for nucleation. However, due to the slow Ni(acac)2 decomposition, relatively few seeds are formed when compared to an approach employing an external reducing agent. The low seed concentration leads to large particles. Moreover, as decomposition kinetics increase at higher temperature, the rate of monomer formation is also increased. If the monomer concentration exceeds the threshold concentration required for supersaturation, nucleation will occur resulting in the formation of new seeds. The formation of new seeds during the growth of existing seeds is the main cause of the broad particle size distribution. With our seed-mediated approach, we obtain a rapid increase in monomer concentration at low temperatures which leads to homogeneous nucleation. These particles maintain their narrow size distribution upon increasing the temperature to 220 °C. Further addition of Ni(acac)2 under decomposition conditions maintains a low monomer concentration and grows the existing particles rather than nucleating new ones. Overall this approach allows a better control of NiNP synthesis. In contrast, addition of Ni(acac)2 at 90 °C did not result in the formation of larger particles, but in a higher yield of NiNP (see the ESI†), confirming that the low-temperature seed formation must be combined with the high-temperature particle growth to obtain larger particles. To the best of our knowledge, this is the first report of seed-mediated NiNPs able to control nanoparticle growth below 10 nm, with earlier studies reporting particles larger than 25 nm.17
Sample | Solvent | wt% Ni | d 1 (±), nm |
---|---|---|---|
Ni/SiO2-h | Hexane | 2.1 | 3.4 (0.5) |
Ni/SiO2-t | Toluene | 0.7 | 3.7 (0.7) |
Ni/SiO2-c | CHCl3 | 1.2 | 3.7 (0.7) |
Ni@SiO2 | CHCl3/H2O | 1.2 | 3.7 (0.7) |
TEM images obtained for directly deposited NiNPs after reductive treatment at 450 °C are presented in Fig. 5a–c. The images highlight the differences in the aggregation of the Ni phase. A weak interaction between the commercial SiO2 and colloidal NiNPs led to ineffective anchoring of the NiNPs, as evident from the sintering after reduction. In contrast, encapsulated nanoparticles (Fig. 5d) retained their initial particle size (3.5 ± 0.5 nm), even after reduction at 550 °C.
To verify the potential of these samples for catalysis, they were employed in the gas-phase benzene hydrogenation to cyclohexane. This reaction, regarded as structure-insensitive, probes the hydrogenation properties of the supported colloidal nanoparticles. Fig. 6 shows turnover frequencies (TOFs) measured at 100 °C normalized to the total Ni content for the supported and encapsulated NiNPs. Hexane deposited NPs were not studied due to the significant sintering observed by TEM. After reduction at 450 °C, the encapsulated NiNPs were more active than the directly deposited particles. Pre-calcination of directly deposited NiNPs did not improve the catalytic performance of these materials (ESI†). Clearly, encapsulation of NiNPs yielded superior performing catalysts compared to direct deposition, showing significantly higher hydrogenation activity after catalysts were reduced at 450 °C. We also found that reduction at 550 °C led to even higher activity for the encapsulated NiNPs, whereas this treatment strongly decreased the performance of the deposited NiNP catalyst. The high activity after reduction at 550 °C should be due to a higher reduction degree, whilst this positive effect is suppressed by sintering for the deposited NiNP catalyst. Although sintering was observed for Ni/SiO2-t, this sample surprisingly was not active at all. Based on these results, we conclude that supporting the NiNPs by encapsulation is the most viable approach to study particle size effects in supported Ni catalysts and proceeded to investigate this synthetic route in greater detail.
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Fig. 6 Gas-phase benzene hydrogenation TOFs at 100 °C over encapsulated Ni@SiO2, Ni/SiO2-c and Ni/SiO2-t after reduction at 450 °C and 550 °C. |
Sample | Ni wt%a | BET (m2 g−1) | V tot (cm3 g−1) | Pore sizeb (nm) | H2 chem. (mmol g−1) | Accessible metallic Ni (%) | d (nm) | |
---|---|---|---|---|---|---|---|---|
H2 chem. | HAADF-STEMc | |||||||
a Determined with ICP-OES after calcination at 500 °C. b Determined from d-spacing using the position of the SiO2 (100) diffraction obtained from low-angle XRD measurements. c Samples were reduced at 600 °C (10 vol% H2) and passivated at RT (1 vol% O2, 6 h). | ||||||||
Ni(4.4) | 2.4 | 979 | 1.46 | 4.4 | 0.019 | 9.1 | 11.1 | 4.3 (± 0.6) |
Ni(5.0) | 4.8 | 983 | 1.74 | 4.9 | 0.052 | 12.9 | 7.9 | 4.6 (± 0.6) |
Ni(6.8) | 3.7 | 964 | 2.15 | 4.7 | 0.036 | 11.4 | 8.9 | 4.7 (± 0.7) |
Ni(7.2) | 8.6 | 891 | 1.18 | 5.4 | 0.087 | 11.8 | 8.6 | 4.6 (± 0.6) |
Further characterization with XRD (Fig. 7) showed that the catalysts were largely amorphous after calcination. The broad reflection around 22° is characteristic of amorphous silica. NiO reflections were only observed for the higher loaded Ni(7.2)@SiO2 and to a lesser extent Ni(5.0)@SiO2 catalysts. Sharp reflections from (200) and (220) planes were observed around 43.7° and 64.0°, respectively, indicating the formation of large NiO crystallites (JCPDS no. 47-1049), which we verified with HAADF-STEM (ESI†). Moreover, very weak and broad contributions centered around 35.2° (envelope of two reflection peaks) and 61.0° are indicative of a Ni-silicate phase (JCPDS no. 49-1859).63,64 This was a first indicator that the nanoparticle-like structure of NiNPs is lost during calcination. Low-angle XRD measurements (Fig. 7b) confirmed the presence of MCM-41 like mesoporous structures in all catalysts. The average mesopore size was calculated from the d-spacing derived from the position of the (100) reflection and ranged from 4.4 nm for Ni(4.4)@SiO2, to 5.4 nm for Ni(7.2)@SiO2 (Table 3).
![]() | ||
Fig. 7 (a) Wide angle XRD patterns of encapsulated NiNPs after calcination at 500 °C (10 h, 1 °C min−1). (b) Small-angle XRD confirming the presence of MCM-41 like mesopores for all catalysts. |
Crucial to the catalytic activity of Ni-based hydrogenation catalysts is the reducibility of Ni and the availability of metallic Ni active sites. Fig. 8 shows the TPR profiles of encapsulated nanoparticles after calcination. All catalysts exhibit a maximum reduction temperature between 600–650 °C, which is characteristic of Ni strongly interacting with the support. Shoulders around 450 °C can be attributed to the reduction of NiO weakly interacting with SiO2. Moreover, the total hydrogen consumption scales with the total Ni content, whilst the TPR profiles are composed of similar features.
Further verification that the Ni was encapsulated after reduction was achieved with XPS depth-profiling. Fig. 9 shows surface Ni/Si molar ratios upon successive Ar+ etching. Samples were first reduced ex situ at 600 °C in 10 vol% H2 in He and passivated in 1 vol% O2. After Ar+ etching for 60 s, all samples exhibited higher Ni/Si ratios, which confirmed an increase in the Ni content below the support surface. This trend continued with every etching dose, although samples with lower overall Ni content saw the Ni/Si ratios plateau after 2–3 doses.
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Fig. 10 HAADF-STEM images and particle size distribution of (a) Ni(4.4)@SiO2 (b) Ni(5.0)@SiO2 (c) Ni(6.8)@SiO2 and (d) Ni(7.2)@SiO2 catalysts after reduction at 600 °C (50 nm scale bar). |
All catalysts were active within the studied temperature range, showing a typical Arrhenius behavior of the conversion at low temperature and deviation from this trend due to the approach to equilibrium at higher temperature (Fig. 11a). No hydrocarbons other than CH4 were detected. Turnover frequencies (TOFs) normalized to surface Ni content were calculated under differential conditions (<10% conversion) at 250 °C (Table 4). No CO formation was observed under these conditions (Fig. 11b). The TOFs revealed that there was no significant difference in catalytic activity, which can be expected as the encapsulated catalysts are almost identical apart from their Ni content. These TOFs are comparable to those reported in literature for Ni/SiO2 systems.65,66 Identical apparent activation energies were also determined for encapsulated catalysts (∼75 kJ mol−1) which is in line with literature values.65–68 These results confirm that there are no adverse effects on the Ni activity by encapsulating the particles in mesoporous silica, and that the catalysts were free from mass transfer limitations.
Sample | Conversion (%) | CH4 selectivity (%) | TOFs (10−3 mol CH4 per mol surface Ni per s) | E appact (kJ mol−1) |
---|---|---|---|---|
Ni(4.4)@SiO2 | 1.3 | 100 | 7.0 (± 0.4) | 75 |
Ni(5.0)@SiO2 | 2.9 | 100 | 5.7 (± 0.02) | 75 |
Ni(6.8)@SiO2 | 2.0 | 100 | 5.7 (± 0.09) | 74 |
Ni(7.2)@SiO2 | 5.7 | 100 | 6.7 (± 0.03) | 77 |
Similar conversion trends were observed during the stability study at 350 °C (Fig. 11c) in which all catalysts were found to be stable for 70 h. Catalysts with a lower Ni content exhibited higher CO selectivities. The catalyst with the lowest Ni content, i.e. Ni(4.4)@SiO2, had a CO selectivity of 43–47% during the entire study. In contrast the highest loaded catalyst, Ni(7.2)@SiO2, had a CO selectivity below 10% throughout the stability test (Fig. 11d). The slight increase in CO selectivity for Ni(4.4)@SiO2, Ni(5.0)@SiO2, and Ni(6.8)@SiO2 catalysts during the stability test may indicate that some of the particles on the external SiO2 surface sintered under reaction conditions. Earlier studies have shown that larger Ni particles have a higher selectivity towards CO.69
To verify whether Ni dispersion changed during the catalytic reaction, spent catalysts were analyzed with HAADF-STEM. Fig. 12 shows HAADF-STEM images of Ni(4.4)@SiO2 (2.4 wt% Ni) and Ni(7.2)@SiO2 (8.6 wt% Ni), i.e. the catalysts at the extreme ends of the initial colloidal particle size and metal loadings, after 70 h CO2 methanation. For Ni(4.4)@SiO2, evidence of particle aggregation was found, although there were clearly also particles that were identical to the initial particle size. This suggests that some particles were not encapsulated and their mobility under reaction conditions led to some sintering. In contrast, encapsulated NiNPs (Fig. 12a, circled) retained their original particle size. This was also observed for Ni(7.2)@SiO2 (Fig. 12b) and the remaining Ni(x)@SiO2 catalysts (see ESI†), which had a higher Ni loading and showed no evidence of particle aggregation. Moreover, we observed significant areas in Ni(4.4)@SiO2 that did not contain NiNPs. We anticipate therefore that with an encapsulation approach in which SiO2 is grown around the NiNPs, Ni catalysts with loadings significantly higher than 8 wt% should be attainable without nanoparticle sintering. Such an approach appears more promising than methods like impregnation or chemical vapor deposition in mesoporous silica or other zeotype materials, in which the possibility of Ni deposition outside of mesopores and cavities (i.e., on the external crystal surface) and Ni aggregation are more difficult to control.42,70,71 Across all samples, particle sizes remained essentially unchanged, with sintering attributed to unencapsulated nanoparticles.
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Fig. 12 HAADF-STEM images of (a) Ni(4.4)@SiO2 and (b) Ni(7.2)@SiO2 catalysts after exposure to CO2 methanation conditions. |
Footnotes |
† Electronic supplementary information (ESI) available: Synthesis procedures and additional material characterization including TEM, XPS (quantification and sputtering results), TGA profiles, N2 physisorption isotherms, and HAADF-STEM images. See DOI: 10.1039/c9cy00532c |
‡ Present address: Inorganic Systems Engineering group, Department of Chemical Engineering, Delft University of Technology, Van der Maasweg 9, 2629 HZ, Delft, The Netherlands. |
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