Open Access Article
Feng Gua,
Guoqing Xiaoa,
Qiuyao Jiaoa,
Yan Liu*b,
Pengyong Weia and
Lei Li
*a
aSchool of Chemistry and Chemical Engineering, Yancheng Institute of Technology, Yancheng, 224051, PR China. E-mail: lee_ycit@hotmail.com
bState Key Laboratory of Coal Conversion, Institute of Coal Chemistry, Chinese Academy of Sciences, Taiyuan 030001, Shanxi, PR China. E-mail: liuyan@sxicc.ac.cn
First published on 5th January 2026
The supported metal catalyst featuring highly dispersed active species poses a challenge for industrial catalysts, even at high loadings. Herein, highly dispersed supported cobalt catalysts were prepared using an impregnation and vacuum-heating strategy. During the vacuum-heating process, coordinated H2O was removed, restricting the formation of metal-bound OH species and their aggregation, yielding small metal oxide species. The synthesized catalyst shows high cobalt time yield and improved C5+ selectivity compared to the catalyst prepared by the traditional impregnation-calcination method. It revealed that more accessible active sites and strong metal–support interaction contributed to superior FTS performance. This study provides a simple, efficient way to prepare supported metal catalysts with high dispersion at an industrial scale.
In the past decade, various classic strategies have been employed in the synthesis of highly dispersed metal catalysts, such as sol–gel method,5,6 colloidal synthesis,7,8 deposition precipitation,9,10 electrostatic adsorption,11 encapsulated structures,12–15 or plasma treatment.16,17 Despite these strategies being effective, they suffer from inherent disadvantages, including complex synthetic steps, low synthetic yield, excessive chemical use, and difficulty in scaling up. To date, the impregnation method remains the preferred synthetic route in the chemical industry due to its ease of scale-up.18 However, metal (oxide) aggregation is inevitable via an impregnation method even with a low loading (<5 wt%). To address this issue, the Krijn P. de Jong group developed highly dispersed supported metal (oxide) catalysts by carefully controlling the drying process19 or the heating atmosphere.20 Drying at 100 °C (the optimum temperature) in N2 flow resulted in the maximum spacing of the Co3O4 nanoparticles, leading to high dispersion rather than aggregation. A calcination atmosphere containing 1% NO/He could prevent the rapid decomposition of cobalt precursors, yielding Co3O4 particles with a diameter of 4–5 nm at relatively high loadings. Besides, the surfactant and metal precursor were introduced into the support via an impregnation method, in which the surfactant was converted into a carbon source that coated the metal nanoparticles, preventing their sintering during calcination.21,22 Similarly, a metal–organic ligand rather than a surfactant was used to construct highly dispersed supported metal catalysts.23–27 On the one hand, the metal precursors and organic ligands are sequentially loaded onto the support, and the interaction effectively inhibits precursor decomposition and the growth of metal oxide nanoparticles.26,27 On the other side, organometallic complexes or coordination compounds react with well-defined surfaces (e.g., oxides, metal nanoparticles, carbon materials) to achieve the target functionalities on the surface.23 By combining grafting of precursors on surfaces via surface organometallic chemistry with a thermolytic, nonoxidative procedure that removes all organic ligands, isolated atoms may be produced on the surface. However, the use of both ligands and surfactants further increases the complexity and cost of the experiment. Accordingly, developing a general and simple method to prepare supported metal catalysts with high dispersion is highly desirable.
Fischer–Tropsch Synthesis (FTS) is an effective catalytic process for high-value-added chemicals and clean liquid fuels. It is well accepted that cobalt-based catalysts show significant advantages of high activity and selectivity for the production of long-chain hydrocarbons.28 The FTS catalytic performance strongly depends on cobalt dispersion, reducibility, and stability. Therefore, the balance between particle size and metal loading, which correlates with metal reducibility and availability, is very important for maximizing activity.
In this study, we propose a simple, highly effective strategy for preparing well-dispersed supported Co nanocatalysts via impregnation followed by vacuum calcination. As illustrated in Fig. 1a, the supported metal catalysts were first prepared by impregnation and dried at low temperature, forming the same precursor/support. Then, it was further calcined by air- and vacuum-heating, respectively. Apparently, the highly dispersed supported metal catalysts were realized using a vacuum-heating strategy rather than an air-heating strategy. This phenomenon should be ascribed to the removal of coordinated H2O in a vacuum-heating environment, which restricts the formation of metal-bound OH species and their aggregation behavior. The resulting small metal oxide species were not agglomerated into larger particles because of their low mobility and high melting point.29 It is evident that the immediate removal of water is very important during the preparation process, especially during the whole heating process. In fact, simple vacuum drying could not completely remove coordinated H2O at low temperatures (e.g., 120 °C), whereas complete removal was achieved at high temperatures (e.g., 450 °C).20 Meanwhile, it was also indicated that the O2-free atmosphere significantly reduced aggregation and sintering. Ingeniously, the vacuum-heating strategy proposed in this study can achieve complete and immediate removal of coordinated H2O and provide an O2-free calcination environment, effectively reducing the aggregation/sintering of active components on the support.
Fig. 1c displays the N2 adsorption–desorption isotherms and the corresponding pore size distribution curves of the representative catalysts (Co/SiO2-V and Co/SiO2-A). Both samples exhibit similar type IV isotherms and hysteresis loops at high relative pressures, indicating the presence of stacked pores.30 As listed in Table S1, there exists a slight distinction of surface area, pore volume, and pore size distribution in the serial contrast samples. For instance, the surface area, pore volume, and pore size distribution are ca.140 m2 g−1, 0.6 cm3 g−1, and 17.5 nm for both Co/SiO2-V and Co/SiO2-A samples. As for Co/Al2O3-V (or Co/ZrO2-V) and Co/Al2O3-A (or Co/ZrO2-A) catalysts, they show similar physicochemical properties.
The morphology, structure, and elemental composition of the representative samples (Co/SiO2-V and Co/SiO2-A) were studied by TEM and EDS. As shown in Fig. 2, there is an obvious aggregation in the Co/SiO2-A sample obtained by air-heating, while there is no obvious agglomeration of cobalt oxides in the Co/SiO2-V sample (Fig. 2a and b). This finding is consistent with XRD analyses. Besides, lattice fringes with interlayer spacings of 0.246 nm and 0.467 nm, corresponding to the (311) and (111) crystal planes of Co3O4, were identified (Fig. S2). Seen from the EDS mappings (Fig. 2c–h), the dispersion of cobalt oxides in the Co/SiO2-A sample is poor, while it exhibits a good dispersion in the Co/SiO2-V sample. It indicates that the vacuum-heating strategy can effectively inhibit the agglomeration of cobalt species, improving its dispersion and providing more accessible active sites.
The surface chemical states of cobalt species were further investigated using XPS. In Fig. 3a, the Co 2p2/3 spectra were deconvoluted into three peaks, corresponding to Co3+, Co2+, and the satellite structure of Co2+. Evidently, the intensity of Co2+ satellites peaks in the Co/SiO2-V sample is stronger than that in the Co/SiO2-A sample. Seen from peak-fitting results (Table S2), the surface molar ratio of Co2+/Co3+ in Co/SiO2-V (0.96) is still larger than that in Co/SiO2-A (0.81). A previous study indicated that this satellite peak should be ascribed to Co2SiO4 rather than surface cobalt species,31 implying a strong metal–support interaction. This strong interaction could effectively prevent the mobility of active cobalt species, significantly enhancing the long-term stability in the FTS reaction.26 In Table S2, the surface atomic concentration of Co (2.42 at%) and Co/Si atomic ratio (0.08) in Co/SiO2-V sample are larger than those in Co/SiO2-A sample (1.22 at% and 0.04). This result reflects a higher number of exposed Co metal sites in the Co/SiO2-V sample.32 More surface-exposed Co metal sites can contribute to superior FTS performance.
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| Fig. 3 (a) Co2p XPS spectra, (b) H2-TPR profiles, (c) H2-TPD profiles, and (d) FTIR of CO adsorption of different Co/SiO2 samples. | ||
The redox property was measured using H2-TPR. Fig. 3b displays the H2-TPR profile of the contrast samples (Co/SiO2-V and Co/SiO2-A). The reduction peaks are mainly located in the low-temperature range (200–500 °C) and the high-temperature range (above 500 °C). The former corresponds to the continuous reduction from Co3+ to Co2+ and Co0, while the latter corresponds to the Co species strongly interacting with silica or CoSi2O4 species.30 We also note that the Co/SiO2-V has a lower reduction temperature but with a small amount of hydrogen consumption compared with the Co/SiO2-A sample. This phenomenon might be linked to the dual effects of highly dispersed, strongly interacting cobalt species coexisting on the catalyst support. Besides, the H2-TPR profiles of different Co/Al2O3 and Co/ZrO2 catalysts were also illustrated in Fig. S3. Similarly, the redox behavior also occurs on Al2O3-supported cobalt catalyst, especially the high-temperature reduction peak, which should be ascribed to a strong interaction between cobalt and alumina or the formed CoAl2O4 species.26 Due to the weak metal–support interaction, only low-temperature range reduction peaks were observed on ZrO2-supported cobalt catalysts. In general, this vacuum-heating strategy effectively boosts the dispersion of cobalt species and their reduction.
Fig. 3c shows the H2-TPD profiles in the representative Co/SiO2-V and Co/SiO2-A samples, and the hydrogen desorption amounts are placed in Table S3. Clearly, the hydrogen desorption amount of Co/SiO2-V (38.9 µmol g−1) is more than that of Co/SiO2-A (16.9 µmol g−1), implying a significant increase in the number of accessible metallic cobalt sites on the surface. The cobalt atomic dispersions are 0.50% and 1.15% for the Co/SiO2-A and Co/SiO2-V samples, respectively. This result correlates well with the above characterizations. Besides, a CO adsorption experiment was performed at room temperature, as detected by in situ FTIR (Fig. 3d). The bands at 2173 and 2116 cm−1 correspond to gas-phase CO adsorption. The bands at 2070 and 2025 cm−1 are attributed to the linear adsorption of CO, while the peak at 1934 cm−1 is caused by the bridge adsorption of CO.33 Notably, the absorption peak intensity of CO in the Co/SiO2-V sample is stronger than that in the Co/SiO2-V sample. It indicated that the Co/SiO2-V sample contains more small cobalt particles, and CO adsorption on small Co particles is significantly stronger than on large Co particles.34 This is because smaller Co particles contain more low-coordination Co atoms, which interact strongly with CO and have a smaller desorption equilibrium constant.
Fig. 4 shows the FTS activity of different catalysts; the detailed results are listed in Tables 1 and S3. As shown in Fig. 4a, the cobalt-based catalysts prepared by the vacuum-heating strategy are obviously superior to those prepared by air-heating. Due to the different nature of the supports, significant differences in FTS activity are observed, and CO conversion activity follows the order: Co/SiO2 > Co/Al2O3 > Co/ZrO2. Especially for the Co/SiO2 catalyst, the stabilized CO conversion is ca. 82.0% in Co/SiO2-V catalyst at a reaction time of 72 h, and the activity is nearly double that of Co/SiO2-A (ca. 43.0%). Accordingly, the mass-specific cobalt time yield (CTY) (3.19 × 10−5 molCO gCo−1 s−1) and TOFs (4.43 × 10−3 s−1) in Co/SiO2-V catalyst are significantly higher than those of Co/SiO2-A catalyst (1.61 × 10−5 molCO gCo−1 s−1, 3.33 × 10−3 s−1). As shown in Fig. 4b, the catalysts prepared by vacuum-heating have higher CTY values than the ones prepared by air-heating. Based on the above characterizations, it can be concluded that the super FTS activity strongly depends on the increased number of cobalt active sites, originating from the vacuum-heating strategy. In addition, the strong metal–support interaction, along with the formation of an inactive metal–support spine species (i.e., CoSi and CoAl), would change the geometric structure of the active site.35 The more efficient utilization of the cobalt–support interface could result in a sharp increase in CTY value. Similarly, for other supports (Al2O3 and ZrO2), catalysts prepared by the vacuum-heating strategy consistently improve or sustain catalytic activity compared to those prepared by the air-heating method, demonstrating the effectiveness and universality of this strategy for preparing highly supported metal catalysts.
| Catalyst | Conv. (CO)a/% | S(CH4)/% | S(C2–C4)/% | S(C5+)/% | H2 desorbed (µmol g−1) | Dispersionb (%) | CTY (10−5 molCO/(gCo s−1)) | TOFsc (10−3 s−1) |
|---|---|---|---|---|---|---|---|---|
| a The data of the seventh day (stable for 72 h) were selected. Reaction condition: T = 200 °C, P = 2 MPa, GHSV = 1000 h−1, H2/CO = 2.b The H2 desorption amounts and dispersion were calculated from H2-TPD results.c The TOF values were calculated by the conversion rate and metal Co dispersion. | ||||||||
| Co/SiO2-A | 43.66 | 7.31 | 8.77 | 83.91 | 16.9 | 0.50 | 1.61 | 3.33 |
| Co/SiO2-V | 81.86 | 3.63 | 4.03 | 92.34 | 38.9 | 1.15 | 3.19 | 4.43 |
The CO-TPD profiles over the contrast catalysts were measured (Fig. S4). The desorption peaks were mainly centered at 50–150 °C and 200–600 °C, corresponding to the desorption of CO molecules (COads) and the CO (CO*) through the recombination of dissociated C* and O*, respectively.33,36 Notably, the CO desorption peak in Co/SiO2-V shifts to a lower temperature compared with Co/SiO2-A. It indicates that there exists fast dissociation and recombination behavior of C* and O* in Co/SiO2-V catalyst, which might improve FTS activity through carbide mechanism.37 Besides, the selectivity of products over different catalysts was also listed in Tables 1 and S3. We found that the Co/SiO2-V catalyst favors the yield of long-chain hydrocarbons (C5+ selectivity = 92.34%) while suppressing methane formation (CH4 selectivity = 3.63%). By comparison, the Co/SiO2-A catalyst exhibits lower C5+ selectivity (83.91%) and higher methane selectivity (7.31%). Similar results were also observed for Al2O3- and ZrO2-supported catalysts. It was reported that the optimum cobalt particle size (6–10 nm) could affect the selectivity of C5+ with a critical value.35 Thus, the superior selectivity of the vacuum-heating prepared catalysts should be assigned to the higher density of metallic cobalt sites and the modified surface structures, which potentially facilitate the chain growth for long-chain alkanes. In addition, some representative Co-based catalysts for the FTS were listed in Table S4. Although the previously reported catalysts were evaluated under different reaction conditions, our as-prepared catalysts exhibited high CO conversion and high selectivity for long-chain paraffins.
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