Lisheng
Guo
*ab,
Peipei
Ai
b,
Xinhua
Gao
c,
Hao
Wu
a,
Xianbiao
Wang
a,
Yasuharu
Kugue
d,
Jiaming
Liang
d,
Weizhe
Gao
d,
Xiaoyu
Guo
d,
Jian
Sun
*e,
Song
Sun
*a and
Noritatsu
Tsubaki
*d
aSchool of Chemistry and Chemical Engineering, Anhui University, Hefei, Anhui 230601, China. E-mail: lsguo@ahu.edu.cn; suns@ustc.edu.cn
bState Key Laboratory of Clean and Efficient Coal Utilization, Taiyuan University of Technology, Taiyuan 030024, Shanxi, China
cState Key Laboratory of High-efficiency Utilization of Coal and Green Chemical Engineering, College of Chemistry & Chemical Engineering, Ningxia University, Yinchuan 750021, China
dDepartment of Applied Chemistry, School of Engineering, University of Toyama, Gofuku 3190, Toyama 930-8555, Japan. E-mail: tsubaki@eng.u-toyama.ac.jp
eDalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian 116023, China. E-mail: sunj@dicp.ac.cn
First published on 12th April 2023
The key to efficient thermocatalytic conversion of CO2 lies in the rational design of catalysts. In this work, Fe-based catalysts supported by different carbon materials (AC, GA, CNF, and MPC) were rapidly synthesized with the assistance of microwave heating. Compared with other supports, small-sized active precursors are coated by graphitic carbon layers for GA-supported Fe catalysts, which will slow down the sintering of particles. Small-sized Fe nanoparticles supported by GA present a benign carburization behavior and water removal ability, which play an important role in stabilizing active carbides and improving product selectivity. These features make GA a more promising support material. In addition, for the catalyst obtained by high-temperature calcination, the size of the active precursor is larger than that obtained by microwave heating, and it is easily coated by amorphous carbon shells, whereas for the small active phase precursor obtained by microwave heating treatment, it is encapsulated by graphitic carbons first, and then the amorphous carbon shells gradually appear around the active carbides with the increase in particle size. The carbon-confined environment provides a stable space for steering CO2 hydrogenation to heavy hydrocarbons. As a result, the rational catalyst exhibits favorable performance. Under relevant industrial conditions (320 °C, 2.0 MPa, 5 g h mol−1), the optimized K–Fe/GA-W-10 catalyst achieves a C5+ selectivity of 53.2% at CO2 conversion of 23.1% and presents a benign stability.
Broader contextThe transformation of CO2 into energy-rich fuels and valuable chemicals is a huge challenging and hot research topic. The critical bottleneck of this process lies in the difficult activation of inert CO2 molecules and poor chain growth ability. Efficient catalyst preparation is one of the key strategies to solve this problem and for potential industrial applications. At present, conventional catalyst synthesis requires high-temperature calcination to obtain the precursor, which usually consumes a good chunk of time. In addition, high-temperature calcination will also destroy the special structure of the catalyst. To overcome this huge challenge, we designed microwave-assisted carbon-confined iron nanoparticle catalysts for steering CO2 hydrogenation to heavy hydrocarbons. The high-temperature treatment lasts only a few seconds, and this method promotes the formation of ultra-high dispersion active metal sites. Moreover, the carbon-confined structure is conducive to CO2 conversion, and maintains the active phase stably. Consequently, the tailor-made catalyst presents benign performance. The present research provides new insights for the rapid fabrication of high-performance catalysts for practical industrial applications in catalytic conversions of C1 small molecules to high value-added chemicals. More importantly, the unique encapsulation and uniform dispersion of active sites from the microwave heating technology have good reference significance for other supported catalysts. |
Iron as a typical catalyst can in situ form two types of active sites under CO2/H2 conditions, including Fe3O4 for reverse water–gas shift (RWGS) and carbides (FexCy) for chain growth, and they have been widely applied for CO2 hydrogenation via modified Fischer–Tropsch synthesis (FTS). Generally, a single iron catalyst without any regulation presents a poor catalytic performance such as low catalytic activity and high light hydrocarbon selectivity, far from needs and expectations. To address this issue, a series of tailor-made iron-based catalysts were synthesized by regulating COx adsorption, electronic environments of active sites, interaction between active metal and support materials, etc. A common means is to introduce electronic promoters in the iron-based system, usually referring to alkali metals (Li, Na, and K), alkaline-earth metals (Mg, Ca, and Sr), and transition metals (Cu, Mn, Zn, Zr, Mo, V, and Nb). Given the excellent promotional effects, K and Na promoters are widely selected for modifying iron-based catalysts to achieve benign catalytic performance. The existence of Na or K above can enhance the surface alkalinity, promoting the adsorption of COx molecules.19 With the incorporation of promoters such as Na, delocalized electrons are transferred from the electronic promoter to the interface of iron carbides, making the surface of iron carbides electron rich.20 CO activation on carbides occurs via Fe–C σ-bonding and the simultaneous back-donation of iron species valence electrons into the 2π* orbital of CO.21 The enhanced electron density of carbides derived from electron transfer is able to intensify the Fe–C bond and weakens the C–O bond.22 Besides, more carbides are formed with the introduction of alkali metals.23,24 Unlike the Na promoter, it is accepted that K is more suitable for the formation of long-chain hydrocarbons.19,24–27
Apart from the promoter modification, controlling the interaction between the active metal and the support is adopted as another important means.28,29 Conventional oxide supports such as Al2O3, SiO2, and TiO2 have been widely used in Fe-based catalysts for CO2 conversion. However, a strong interaction between Fe and the oxide support may form a hardly reducible iron species (for example, iron silicates) and inhibit the reduction and carburization of an active Fe phase during the CO2 hydrogenation. Furthermore, various types of carbonaceous supports such as carbon nanofibers (CNFs), mesoporous carbons (MPCs), activated carbons (ACs), and graphenes (GAs) have been regarded as promising catalytic supports due to their tunable surface properties, thermal stability, and weak metal–support interactions.22,30–33 Although some advances have been reported, carbonaceous materials as promising supports have not yet received enough attention in the process of CO2 hydrogenation to long-chain hydrocarbons, let along the differences of promotional effects among different carbonaceous supports. Previously, we have designed supported iron nanoparticles for FTS by utilizing “microwave dielectric heating” effects, in which iron species presents benign dispersion.34 Microwave energy, when incident on a lossy dispersive material, generates heat within the material via the interactions of the electromagnetic field with the material's molecular and electronic structures. According to the Poynting theorem, the total power entering a volume V through the surface S goes partially into increasing the field energy stored inside V and is partially lost into heat.35 It can be judged that the ability of a material to heat up in the presence of an electromagnetic wave depends on the nature of its interaction with electric and magnetic components of the field. Generally, carbonaceous materials (graphite, graphenes, etc.) are dielectric absorbers having a sp2 bonded carbon network, which contains copious amounts of delocalized π electrons, which in the presence of an external electric field, start moving in the direction of the field and generate an electric current. As the electrons cannot couple to the changes of phase of the electric field, energy in the form of heat is dissipated. This process is referred to as interfacial polarization (also known as the Maxwell–Wagner–Sillars effect).36–38
In this work, a series of carbon material (including GA, CNF, AC, and MPC)-supported iron nanoparticles were prepared for CO2 conversion, where the precursors were treated by rapid microwave heating (MH). The improved dispersion, carburization behavior, and water removal ability are responsible to the high selectivity of long-chain hydrocarbons. Thereinto, a small-sized Fe nanoparticle encapsulated in a carbon shell is a key feature structure, which effectively stabilizes the carbide active phase and provides a favorable carbon environment. Correspondingly, a GA-supported Fe nanoparticle catalyst reaches C5+ selectivity as high as 53.2% at CO2 conversion of 23.1% (Scheme 1).
Scheme 1 Schematic diagram of the synthesis of different catalysts via facile microwave heating treatment. |
In addition, in order to investigate the effect of microwave treatment time, the catalysts treated for different microwave time periods were prepared, marked as K–Fe/GA-W-t (t = 0, 5, and 15 s). Meanwhile, a K–Fe/GA catalyst was also fabricated via muffle calcination at different temperatures (T = 550, 700, or 850 °C for 5 h) under the protection of N2 atmosphere and labelled as K–Fe/GA-C-T.
By contrast, a SiO2-supported iron catalyst was also fabricated. Similar to carbon material-supported Fe catalysts, same contents of Fe and K were introduced into SiO2 by the same method. Considering that microwave heating could not heat SiO2, the obtained precursor was calcined in a muffle (550 °C for 5 h) under the protection of N2 atmosphere, and the obtained catalyst was labeled as K–Fe/SiO2-C-550.
In situ XRD data were conducted using an Empyrean-100 PANalytical Empyrean-100 373 diffractometer with Cu Kα irradiation. The catalyst was first exposed to a H2 atmosphere for reduction, and the temperature was gradually increased from room temperature to 400 °C. After reduction at 400 °C for 90 min, the temperature was decreased to 320 °C. Subsequently, CO2 and H2 (H2/CO2 = 3) were introduced to the catalyst with a reaction pressure of 1.0 bar. The XRD patterns were collected over time.
N2 adsorption–desorption curves were measured at −196 °C using a NOVA 2200e apparatus to determine the specific surface area based on the Brunauer–Emmett–Teller (BET) method. Before measurement, the catalyst was outgassed under vacuum at 200 °C for 6 h.
A BELCAT-II-T-SP analyser was used to perform the H2-temperature programmed reduction (H2-TPR) and CO2-temperature programmed desorption (CO2-TPD). For H2-TPR, 50 mg catalyst was pretreated at 150 °C with Ar for 1 h. Subsequently, 5 vol% H2/Ar gas mixture was fed into the reactor when the temperature dropped to 50 °C. Finally, the H2-TPR trace was recorded from 50 to 800 °C at a heating rate of 10 °C min−1. As for CO2-TPD, 50 mg catalyst was reduced at 400 °C for 2 h in flowing 5 vol% H2/Ar. After pretreatment, the catalyst was flushed in an Ar flow for 30 min. Then, the temperature was decreased to 50 °C in the Ar flow and saturated with CO2 for 30 min. After flushing in the Ar flow for 30 min, CO2-TPD signals were recorded from 50 to 800 °C at a heating rate of 10 °C min−1.
X-ray photoelectron spectroscopy (XPS) analysis was performed using a Thermo Fisher Scientific ESCALAB 250Xi multifunctional X-ray photoelectron instrument.
Transmission electron microscopic (TEM) images of catalysts were acquired using a JEOL JEM-3200Fs at an accelerating voltage of 100 kV.
Raman spectroscopy measurements were taken using a HORIBA HR Evolution Raman spectrometer with a 2 mW 532 nm excitation laser. The exposure time for each line was 10 s, and the number of exposures was 2.
The static water contact angle was measured using a DSA100M (Theta Flex) in an environmental chamber saturated with water vapor under ambient conditions.
Catalyst | HTa | GHSVb | H2/CO2 | P/MPa | T/°C | CO2 Conv. | CO Sel. | CO-free HCs Sel. (mol%) | Yield (C5+)/% | ||
---|---|---|---|---|---|---|---|---|---|---|---|
CH4 | C2–C4 | C5+ | |||||||||
All the conversion and selectivity data are collected at a stable 6–8 h on stream.a Represents the heating time (HT) over 100 °C during catalyst preparation.b Unit in mL gcat−1 h−1. | |||||||||||
K–Fe/SiO2-C-550 | 5 h | 4800 | 2.5 | 2.0 | 320 | 23.1 | 46.1 | 14.8 | 39.6 | 45.6 | 5.7 |
K–Fe/AC-W-10 | 10 s | 4800 | 2.5 | 2.0 | 320 | 26.3 | 40.2 | 16.4 | 38.9 | 44.7 | 7.1 |
K–Fe/CNF-W-10 | 10 s | 4800 | 2.5 | 2.0 | 320 | 25.6 | 45.7 | 15.2 | 33.0 | 51.8 | 7.2 |
K–Fe/GA-W-10 | 10 s | 4800 | 2.5 | 2.0 | 320 | 23.1 | 42.9 | 13.7 | 33.1 | 53.2 | 7.0 |
K–Fe/MPC-W-10 | 10 s | 4800 | 2.5 | 2.0 | 320 | 24.5 | 46.2 | 21.8 | 37.8 | 40.4 | 5.3 |
K–Fe/SiO2-C-550 | >10 h | 4800 | 2.5 | 2.0 | 320 | 18.9 | 38.7 | 40.8 | 31.2 | 28.0 | 3.2 |
FeK/MWNTs27 | >21 h | 9000 | 3.0 | 2.0 | 340 | 43.6 | 23.4 | 27.1 | 38.5 | 34.4 | 11.5 |
FeK/MPC30 | >21 h | 8000 | 3.0 | 2.5 | 300 | 37.2 | 8.4 | 20.0 | 36.1 | 43.9 | 15.0 |
KFe/NCNT31 | >30 h | 50000 | 3.0 | 2.5 | 360 | 31.8 | 74.6 | 76.1 | 20.1 | 3.8 | 0.3 |
Fe/C–K2CO340 | >34 h | 2400 | 3.0 | 2.0 | 320 | 37.1 | 11.5 | 12.9 | 41.6 | 45.5 | 14.9 |
FeK/C-1EDA41 | >24 h | 2400 | 3.0 | 1.0 | 300 | 20.1 | 31.7 | 17.2 | 43.3 | 39.5 | 5.4 |
In general, the obtained catalysts for the reaction need heating pre-treatment, such as calcination, to obtain the desired structure or phase composition. Previous reports have revealed that long-time high-temperature treatment results in several undesired transformations including active-phase sintering and structure failure, which will cause poor catalytic performance, in turn. Previously, it has been reported that the MH method as a facile operation is able to sharply shorten the heating time and promote the dispersion of active species.34 As a result, the high-temperature pretreatment time for a given catalyst was listed and compared in Table 1. Table 1 only lists the heating processing times above 100 °C. Intuitively, different from the conventional heating procedure, MH treatment can effectively shorten the heating time from several hours to seconds (10 s), which means a shorter preparation cycle and a lower preparation cost. To some extent, the K–Fe/GA-W-10 catalyst obtained by this MH method presents more potential application values.
Meanwhile, the influences of MH time (0–15 s) and calcination temperature (550–850 °C) on CO2 hydrogenation performance over GA-supported Fe catalysts were also investigated (Fig. 1). As for the K–Fe/GA-W-0 catalyst without any heating treatment, it presents a poor C5+ hydrocarbon selectivity. With the prolongation of MH time, the catalytic activity increases slightly while C5+ hydrocarbon selectivity increases obviously. When the microwave time reaches 10 seconds, CO2 hydrogenation shows good performance. On the contrary, calcined catalysts at high temperatures show inferior catalytic hydrogenation performance. Moreover, calcination at high temperatures (850 °C) is not conducive to the formation of C5+ hydrocarbon. Catalytic stability is an essential index for the designed catalyst. As depicted in Fig. 1(c), the K–Fe/GA-W-10 catalyst presents benign stability over 200 h on stream. The C5+ selectivity stably maintains at 53% throughout the test. These results further indicate that the catalyst prepared by MH has a better application prospect than that of the catalyst prepared by conventional calcination in terms of preparation cost and cycle.
Fig. 2 and Fig. S6 (ESI†) show the in situ XRD patterns of different catalysts under the same operating conditions. For the K–Fe/AC-W-10 catalyst, new iron phases ascribed to FeO (JCPDS, 74-1886) and metallic Fe (JCPDS, 85-1410) appear (Fig. 2(a), 400-0). It provides a direct evidence that Fe3O4 was reduced to FeO and then to Fe. As the reduction time expands, the diffraction peak intensity of Fe gradually increases. However, the intensity of metallic Fe decreases when the reactant gas is introduced into the system and a new phase corresponding to Fe3O4 appears. Fe2C and Fe5C2 appear with the proceeding of the reaction. Apart from the obvious peaks of Fe3O4, the peaks of Fe could be clearly distinguished. For K–Fe/CNF-W-10, the diffraction intensity of Fe changes slightly with the extension of reduction process, and a new carbide (Fe5C2) is formed when the reactant gas is introduced. Meanwhile, Fe has the strongest diffraction intensity than that of other phases. It is worth noting that when the reaction proceeds to a certain extent, the change in the diffraction intensity of metallic Fe is almost negligible (Fig. 2(a) and (b)). As far as K–Fe/GA-W-10 is concerned, the content of Fe increases continuously with the proceeding of reduction. However, the diffraction intensity of Fe is sharply decreased after the introduction of reactant gas, and Fe2C is formed under the atmosphere. This indicates that carbides are easier to form in this catalyst. With the reaction proceeding, the dominant phases are Fe3O4 and Fe2C, and the diffraction intensity of Fe becomes very low. For K–Fe/MPC-W-10, the diffraction intensity of Fe increases gradually during the reduction process. When the reactant gas is introduced, Fe is oxidized, resulting in the formation of Fe3O4, and carbides gradually appear as the reaction proceeds. Different from the above-mentioned catalysts, the diffraction peak of Fe3O4 increases gradually with the proceeding of the reaction (Fig. 2(d)). By contrast, the iron species in the K–Fe/SiO2-C-550 catalyst are difficult to be reduced and used for carbonization. The main phases are also Fe3O4 and Fe2O3 (Fig. S6, ESI†).
Fig. 3(c)–(f) and Fig. S9, S10 (ESI†) show the TEM images and the corresponding crystallite sizes of the used samples. After the reaction, K–Fe/AC-W-10 exhibits a core–shell structure, in which the shell is a carbon layer and the core is carbides. The lattice planes of Fe2C (−311) are detected as the main active phases. The particle size of iron species is about 20 nm (Fig. 3(a) and Fig. S10a, ESI†). A similar structure also appears in the K–Fe/CNF-W-10 sample with a larger size (50 nm), and the main phase is Fe5C2 (510). However, for the used K–Fe/GA-W-10 sample, there is no core–shell structure. Notably, iron species present small particle sizes, usually less than 5 nm, which is different from that of other catalysts. For the remaining catalysts, the particle sizes of iron active species increase significantly after the reaction (Fig. S7 and S10, ESI†). In addition, the main phase is Fe2C (121) for K–Fe/GA-W-10. For the K–Fe/MPC-W-10 catalyst, the core–shell structure also appears after the reaction, and the particle sizes change from 40 to 100 nm (Fig. 3(d)). Similar to the K–Fe/GA-W-10 sample, Fe2C (121) remains the dominant phase, which is well consistent with the XRD analysis (Fig. S5, ESI† and Fig. 3(d)). Besides, based on the XRD data shown in Fig. 2, the particle sizes of different catalysts in various time periods are compared and listed in Table S4 (ESI†). Obviously, with the process of reduction, the particle size of iron species increased gradually, and then the catalytic particle meditation decreased when switching to reaction gas. With the extension of the reaction time, the active phase particles gradually increased and stabilized. Similar to the TEM results, the GA-supported catalyst had the smallest particle size of iron species. These findings indicate that the utilization of GA support is conducive to the carburization of Fe3O4, producing small particles of active phases and providing more contact interfaces between active sites and feed gases. Moreover, GA-supported Fe nanoparticles are more conducive to maintaining the small particle size. By contrast, for the used K–Fe/SiO2-C-550, Fe3O4 (220) rather than carbides as the active phase is detected and the sizes counter at 100 nm, which is also confirmed by XRD results (Fig. S6 and S9, ESI†).
The reduction and CO2 adsorption properties were investigated by H2-TPR and CO2-TPD experiments, respectively (Fig. S11 and S12, ESI†). Different from the inert SiO2 support, carbon material-supported Fe nanoparticles are easier to be reduced. Thereinto, the iron species in the K–Fe/AC-W-10 catalyst are more easily reduced, followed by K–Fe/GA-W-10 and K–Fe/MPC-W-10, and finally the K–Fe/CNF-W-10 sample (Fig. S11, ESI†), which is consistent with the results from in situ XRD patterns (Fig. 2). As from H2-TPR, improved reduction behavior can promote the formation of Fe phase and facilitate the in situ formation of active phase. In general, from CO2-TPD, the desorption temperature below 650 °C could be assigned to CO2 chemisorbed peaks and physical adsorption peaks, while the peaks above 650 °C are due to the degradation of carbonaceous materials. Correspondingly, according to the results of CO2-TPD, CO2 raw molecules could interact well with iron species over K–Fe/GA-W-10 and K–Fe/MPC-W-10 catalysts compared to the remaining samples (Fig. S12, ESI†).
The effects of MH time (0–15 s) on the catalyst structures were investigated (Fig. S13, ESI†). For the sample after vacuum drying without any MH treatment, it shows large bulk irregular size structures. With the extension of MH time, bulk structures become small-sized particles, given that the microwave heating action is strengthened. When the microwave time exceeds 10 s, the catalyst particles are obviously reduced and further change is not obvious (ca. 5 nm), and more graphitic carbon layers appear around the metal species. This indicates that the suitable MH time is beneficial for the formation of small-sized iron species. In addition, TEM was performed on the used catalysts treated with different microwave durations (Fig. S14, ESI†). It can be found that a suitable microwave heat treatment duration (10 s) can effectively tune the particle size of active species. The chain growth reaction is a structurally sensitive reaction, and the smaller particle size is helpful to improve the catalytic performance. Meanwhile, in order to further compare the difference between MH and traditional heating methods such as calcination, the microwave and calcined samples were compared (Fig. S15, ESI†). Apparently, high calcination temperatures (700 and 850 °C) render the formation of large particles (Fig. S15b and c, ESI†). Although an appropriate low calcination temperature (550 °C) brings uniform particles, MH treatment is more conducive to the formation of small-sized iron species with high exposed active surface. In addition, the samples with various MH time periods present similar XRD patterns, indicating that MH can effectively promote the uniform dispersion of metal particles (Fig. S16, ESI†). By contrary, the corresponding precursor samples (K–Fe/GA-W-0 or K–Fe/GA-C-0) show obvious differences after the utilization of high-temperature calcination (Fig. S17, ESI†). With the increase in calcination temperature, metallic Fe species appear rather than Fe3O4 in an inert N2 atmosphere. Previously, similar findings were reported for NiO supported on graphene, and this phenomenon may be ascribed to the action of graphitic carbons and hydroxyl groups.43,44 Clearly, rapid heating and slow high calcination can induce different process changes in the catalyst precursor period. It shows that the MH method is not only fast and efficient, but also more beneficial to the preparation and synthesis of specific catalysts.
The phase composition and content of surface species were also investigated by XPS (Fig. 4, Fig. S18–S20, and Tables S5–S7, ESI†). As shown in Fig. S18, the XPS spectrum of the Fe 2p region of all samples can be fitted with two spin–orbit doublets corresponding to the Fe 2p1/2 and Fe 2p3/2 peaks and the corresponding satellite peaks of Fe2+ and Fe3+, which are typical characteristic peaks of Fe3O4.45 The iron nanoparticles supported by GA and CNF have a higher surface Fe(II) content (Fig. S18, ESI†). As mentioned above, the K promoter promotes the formation of heavy hydrocarbons.
Different from the K–Fe/SiO2-C-550 reference catalyst, the content of Fe(II) is higher for carbon-supported Fe catalysts (Fig. S19, ESI†), an active phase for catalyzing CO2 molecule hydrogenation. According to the C 1s and O 1s spectra, there are more C–C species and low content of C–O/CO species, indicating that more adsorption species are converted into hydrocarbon products over K–Fe/GA-W-10 (Fig. S20, ESI†). Notably, the low intensity of Fe species especially for K–Fe/GA-W-10 indicates that iron species are encapsulated into the support or carbon shells (Fig. 3 and Fig. S7, S10, ESI†). This phenomenon could also be confirmed based on the surface content analysis of iron species (Table S8, ESI†). As for the K–Fe/GA-W-10 catalyst, there is no metal species coated by a carbon shell, thus Fe nanoparticles are more likely to be encapsulated in the graphene support or graphitic carbon layers. Based on this discussion, the schematic diagram of the active iron species in/on the support materials is depicted (Fig. 4(d)–(f)). For the used samples, the data of K and Fe surface content were also compared, as shown in Fig. S21 (ESI†). Similar to the samples before the reaction, the samples after reaction showed the same trend, indicating that the packaging structure was still obvious in the reaction process, and gradually appeared for AC- and MPC-supported iron catalysts. As shown in Fig. S22 (ESI†), CO-TPD experiments were further conducted to investigate the Fe accessibility. Compared with K–Fe/GA-W-0, the CO adsorption intensity decreases with the assistance of microwave heating. By contrast, the catalyst with calcination treatment presents inferior CO adsorption at low temperatures. Moreover, the desorption temperature of CO in the high-temperature region increases further. These results further support these findings to some extent (Fig. 4). In addition, the K 2p XPS spectra of used samples were compared, as shown in Fig. S23 (ESI†). As indicated, with the increase in K content, the binding energy shifts to a high binding energy location, indicating that K donates electrons to iron species. Generally, the change in electronic density enhances the strength of the Fe–C bond. In addition, the K promoter can suppress olefin secondary hydrogenation and then promote the formation of heavy olefin-rich hydrocarbons. Meanwhile, it is reported that the contact angle of H2O on graphenes is significantly higher than that on graphite, which indicates that graphenes have the most hydrophobic surfaces with very weak interactions with the H2O molecules.47 Xu et al. also reported that nanoscale zero-valent iron prepared by a carbothermal reduction method catalyzed the amorphous carbon to form hydrophobic graphitic layers.48 Generally, the presence of H2O molecules can oxidize the active phase and thus reduce the CO2 hydrogenation performance. Quick water removal from hydrogenation processes plays a crucial role for promoting COx hydrogenation.25,49 The water contact angle test shows that the graphene-supported catalyst has benign hydrophobicity, and the hydrophobicity of K–Fe/GA after MH treatment is enhanced (Fig. S24, ESI†). However, after the reaction, the hydrophilic and hydrophobic properties will change with the occurrence of the reaction. Thus, Fe nanoparticles encapsulated in the hydrophobic graphene support or graphitic carbon layers could be an ideal sample for catalyzing CO2 hydrogenation.
The differences in the structure of the as-prepared catalysts with different heating manners were further assessed by Raman spectroscopy. In terms of the Raman spectra of three catalysts, two peaks can be clearly seen at around 1580 and 1350 cm−1, which can be attributed to the G band and the D band, respectively (Fig. S25, ESI†).22,50 Thereinto, the intensity of the G band is relative to the growth of graphitic carbons, while the intensity of the D band is a feature for disordered graphite including defects and sp3-hybridized carbons; then, the relative intensity (ID/IG) of the D band and G band can reflect the defect sites or graphitization degree. Obviously, the utilization of different heating methods shows slight influence on the defect structures of supports (Table S9, ESI†), which also means that the GA-loaded iron nanoparticles have benign thermal stability during preparation steps. This finding shows that the GA-supported iron catalyst has good stability, and the difference in catalytic performance is mainly due to the formation of the package structure. In addition, the spent K–Fe/GA-W-10 catalyst obtained after 200 h of reaction was further characterized by TEM. With the prolongation of reaction time, the particle size of the catalyst increases obviously (Fig. 2 and Fig. S26, ESI†). Moreover, the crystalline Fe5C2 core is covered with an amorphous shell, which is distinctly different from the previous catalyst obtained after 6 h of reaction (Fig. S26, ESI†). The core (iron species)–shell (carbon) configuration is a typical structure for FTS Fe-based catalysts.40,51–53 Similarly, Kim et al. also reported this phenomenon for the Na–Fe3O4/CNT after 24 h of reaction.54 Chernyak et al. reported the formation of a carbide core–amorphous carbon–graphitic carbon structure.55 Zhang et al. reported that the presence of a graphene shell could inhibit the sintering and agglomeration of active phases, and reduce the negative effects of water by blocking the contact between H2O and active phases.56 It can be inferred that when the catalyst particle size is small and coated by graphitic carbon layers, the amorphous carbon is not easily formed on the surface of active phases (Fig. 2 and Fig. S10, ESI†). However, when the particle size increases significantly, the catalyst particles show a tendency to form the amorphous carbon (Fig. S26, ESI†). The presence of the graphitic carbon or amorphous carbon can provide a good stable carbon environment for active carbides, making the catalyst exhibit good catalytic performance (Fig. 5). Previously, Gupta et al. reported a carbon-coated core–shell iron nanocatalyst for efficient CO2 hydrogenation, and found that the presence of a carbon shell could prevent rapid deactivation via hindering the aggregation of particles and enhance C2+ olefin selectivity.57 Besides, porous graphene-confined Fe catalysts also presented benign activity and excellent stability for CO2 hydrogenation to C2+ olefins, which is ascribed to the confinement effect.58
Fig. 5 Schematic diagram of the changes in active iron species microenvironment on different catalysts after high-temperature heating treatment and reaction. |
Under such a space-confined carbon environment, the active iron sites are probable to express unique catalytic performance, which finally results in a favorable performance as we observed. When the MH time is 10 s, the K–Fe/GA-W-10 catalyst shows 53.2% C5+ selectivity at a CO2 conversion of 23.1%, and the test of 200 h reaction indicates good stability for CO2 hydrogenation. Carbon material-supported iron nanoparticles with the utilization of rapid MH provide a new and facile strategy for CO2 hydrogenation to produce high value-added products such as heavy hydrocarbons. Excellent absorbents of microwaves such as GA act as benign supports for catalyzing CO2 hydrogenation, and MH distinctly shortens the manufacturing cycle and production cost, which is an important factor in industrial production.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ey00071k |
This journal is © The Royal Society of Chemistry 2023 |