Jinshi Dong*a,
Hongli Yanga,
Shengtong Lia,
Panpan Chang
a and
Jiaqiang Yang
*b
aLaboratory of New Energy and Environmental Catalysis, School of Biological and Chemical Engineering, Guangxi University of Science and Technology, Liuzhou 545006, Guangxi, China. E-mail: jinshidong@gxust.edu.cn
bZhongyuan Critical Metals Laboratory, Zhengzhou University, Zhengzhou 450001, Henan, China. E-mail: jqyang@zzu.edu.cn
First published on 15th July 2025
The hydrogenation of CO2 to methane at atmospheric pressure is a significant chemical approach to achieve carbon neutrality and gain renewable energy. However, developing catalysts with high selectivity and high methane yield remains challenging. In this study, a series of Rh–Al2O3 catalysts with varying Rh particle sizes were prepared by modulating the Rh loading amounts. Rh nanoparticles (Rh NPs) were found to exhibit superior performance compared to Rh single atoms (Rh SAs) under identical reaction conditions. The sharp decrease in CH4 selectivity at high temperature is dominantly attributed to the side reaction of dry reforming of methane instead of the limitation of reaction thermodynamics. It was found that there was the coexistence of formate and CO pathways in CO2 methanation on Rh–Al2O3 catalysts regardless of Rh loadings and formate pathway is dominate for CO2 methanation when the temperature high than 400 °C. Turnover frequency (TOF) calculations indicated that the theoretical CH4 generation frequency of Rh NP was three times higher than that of Rh SA. Kinetic experiments and DFT calculations revealed that the dissociation and activation of H2 is the key factor affecting the performance of Rh–Al2O3 catalyst. This study facilitates our understanding of Rh size-dependent chemistry for CO2 methanation reaction.
The molecular CO2 is very stable and it is a great challenge to convert it to the target product methane with high selectivity. CO2 methanation (eqn (1)) is a strongly exothermic reaction, which means that it will be limited by thermodynamic equilibrium at high temperatures.17,18 The reaction is accompanied by other side reactions such as reverse water gas shift (eqn (2), RWGS) and dry reforming of methane (eqn (3), DRM).19–21 Therefore, a highly active catalyst is essential to overcome high kinetic limitations of CO2 methanation while promoting methanation selectivity. Compared to other supported metals, supported Rh catalysts exhibit excellent catalytic performance and methane selectivity in CO2 methanation reactions.22–27 Previous studies indicated that CeO2, TiO2, ZrO2, and Al2O3 have been used as the support to investigate the catalytic performance of metal oxide-supported Rh catalysts in CO2 hydrogenation, among which the highest CO2 conversion towards methane is obtained for the Rh–Al2O3, benefiting from the strong adsorption capacity of the Al2O3 support for CO2.19,28
CO2 + 4H2 ↔ CH4 + 2H2O; ΔH298K = −165 kJ mol−1 | (1) |
CO2 + H2 ↔ CO + H2O; ΔH298K = 41.2 kJ mol−1 | (2) |
CO2 + CH4 ↔ 2CO + 2H2; ΔH298K = 247 kJ mol−1 | (3) |
It is widely accepted that the CO2 methanation reaction activity and selectivity can be tuned by controlling metal particle size, elemental doping, and metal–support interactions.3,6,23,24,29–36 Karelovic et al.29 reported that larger Rh particles are up to four times more active than smaller particles at low temperature (135–150 °C), whereas at higher temperatures (200 °C) the influence of Rh particle size on catalytic activity is insignificant. A similar phenomenon was found in the Rh–TiO2 catalyst system, but the catalytic properties did not change appreciably when the particle size was increased to about 7 nm.25 Bentrup et al.33 studied the modification of Rh–Al2O3 catalysts with Ni and K to vary their acidity/basicity and redox behavior and found that the Ni modification promotes the formation of CH4, whereas K modification enhances the CO formation. Siang et al.23 showed that the metal–support interaction and the degree of basicity are significantly enhanced with increasing Rh contents, which facilitates CO2 adsorption and reduces the activation barriers (from 110.2 to 19.7 kJ mol−1) during the methanation reaction, thereby promoting catalytic activity.
Despite so much progress up to now, the fundamental factors affecting CH4 product yield still remain highly controversial. In order to gain deeper insights into the influence of particle size on catalytic activity and selectivity, a series of Al2O3-supported Rh catalysts with varying Rh particle sizes were synthesized and subsequently analyzed to reveal the structure–performance relationship for CO2 methanation. Our findings indicate that the adsorption and activation of H2 are critical factors influencing product selectivity and larger Rh particle sizes would facilitate H2 activation, thereby enhancing CO2 methanation activity. The decreased CH4 selectivity at high temperatures is mainly due to the side reaction of dry reforming of methane. Furthermore, in situ infrared spectroscopy studies have demonstrated that both the formate and CO pathways are main reaction pathways for the CO2 methanation reaction catalyzed by the Rh–Al2O3 catalyst.
CO adsorption diffuse reflectance infrared Fourier transform spectroscopy (CO-DRIFTS) was conducted on a Nicolet iS50 FTIR spectrometer equipped with a ZnSe window sample tank in a pike high temperature reaction chamber. Approximately 20 mg of catalyst was loaded into a sample tank, with the bottom surface lined with quartz wool and a metal mesh positioned beneath to prevent the obstruction of the gas outlet. The samples were pretreated by reduction in 5% H2/Ar (100 mL min−1) at 300 °C for 15 min before testing. After cooling to room temperature (RT), the system was purged with Ar for 10 min, and then the spectrum was recorded as the background. Subsequently, a 10% CO/Ar (50 mL min−1) gas flow was introduced into the sample tank and held for 3 min and then the inlet flow was switched to Ar (100 mL min−1) and held for 60 s, afterwards the spectrum was recorded.
In a typical in situ DRIFTS measurement, ∼15 mg of catalyst was used, and the reduction pretreatment and background acquisition operations were the same as above. Afterwards, the reaction atmosphere was introduced. The raw gas of CO2 hydrogenation consists of 1% CO2 and 5% H2 in a balanced mixture with 94% Ar (sourcing from 10% CO2/Ar, 20% H2/Ar and 99.99% Ar, Liuzhou Huaao Gas Company Limited), with a total flow rate of 40 mL min−1. The sample was heated to the target temperature at a rate of 15 °C min−1, held for 2 min, and then the spectra were recorded. The CO-DRIFTS measurement of the spent catalyst after the 400 °C in situ reaction was the same as the method of fresh catalyst after reduction pretreatment.
X-ray photoelectron spectroscopy (XPS) analysis was performed using a Thermo Fisher Scientific K-Alpha spectrometer equipped with a monochromatic Al Kα X-ray source (1486.6 eV) operating at 12 kV. All catalyst samples were promptly transferred to vacuum tubes within an Ar-filled glove box and maintained under specified atmospheric conditions, before XPS testing. The samples were also loaded onto the holder in the glove box to prevent oxidation of Rh states. For XPS characterization of samples before the reaction, the samples were reduced in 5% H2/Ar (100 mL min−1) at 300 °C for 15 min on a Beijing Builder PCA-1200 chemisorption analyzer and cooled down in the reduction atmosphere then kept in sealed centrifuge tube. The spectrum of spent catalyst after 400 °C in situ DRIFTS reaction was also recorded. After the measurements, all binding energies were charge-corrected using the dominant sp2-hybridized carbon component (C–C/C–H) −40 of the C 1s adventitious carbon peak fixed at 284.8 eV. The fitting residual is controlled within ±0.1 eV. XPS peak fitting was performed with XPSPEAK, the baseline used a Shirley non-linear sigmoid-type. Rhodium was analyzed on the 3d5/2 and 3d3/2 doublet separated from 4.84 eV. The ratio of peak areas for Rh 3d5/2 and Rh 3d3/2 is constrained to 3:
2. The fraction of rhodium in a metallic state was evaluated as the ratio between atomic surface concentration of Rh0 and the total Rh concentration (Rh0/Rhtot).
Temperature programmed surface reaction (TPSR) test pretreatment conditions and experimental conditions were consistent with the activity evaluation test. The concentrations of CO2, H2, CO and CH4 were monitored using the HPR-20 R&D online Mass Spectrometer (Hiden Co. Ltd). Prior to the test, the initial gas concentration was calibrated using the quantitative analysis software “QGA Professional” according to the exact flow rate of each gas measured by the mass flowmeter. The kinetic measurements of the CO2 hydrogenation reaction were performed under the condition that CO2 conversion was controlled at a low level (below 20%). In order to prove that our kinetic testing conditions are limited neither by mass transfer nor by heat transfer, we conducted the calculations of Weisz–Prater criteria (CWP) and Mears criteria (CM) for all catalysts with CO2 conversions higher than 20% (uniformly applying the values at 500 °C), and the calculation results show that the mass transfer and heat transfer effects can be entirely ignored in our system. Detailed calculation processes are shown in ESI Note 2.†
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Fig. 1 TEM images of reduced (a) 0.1Rh–Al2O3, (b) 0.5Rh–Al2O3, (c) 1Rh–Al2O3 and (d) 2Rh–Al2O3 catalysts. |
It is also noteworthy that product selectivity showed a tendency towards regular change. At the same temperature, the CH4 selectivity gradually increased and the CO selectivity decreased with the increase of Rh loading, but when Rh loading was increased from 1% to 2%, the CH4 selectivity under the same conditions showed an insignificant increase, and the decrease in CO selectivity was also not obvious. Studies above have indicated that further increases in Rh loading do not result in a significant enhancement in CH4 selectivity and a loading of 1% Rh could represent the optimal condition for the CO2 methanation reaction. Furthermore, methane production was not observed for 0.1Rh–Al2O3 at 300 °C, indicating that Rh NPs exhibit superior CO2 methanation activity compared to Rh SAs at low temperatures.
In order to reveal the difference of intrinsic performance between catalysts with different Rh loadings, we used the temperature programmed surface reaction (TPSR) method to investigate the real-time concentration changes of the reactants CO2 and H2 and the products CH4 and CO. The partial pressure signals of CH4 (m/z = 16), CO (m/z = 28), CO2 (m/z = 44) and H2 (m/z = 2) were recorded by mass spectrometry (MS) in real time from 200 °C to 500 °C, as shown in Fig. 3. It can be observed that the reaction starting temperatures (288 °C, 240 °C, 234 °C and 206 °C, respectively) decreased with increasing of Rh loading, indicating that a higher loading of Rh favors higher reaction activity. Meanwhile, the concentration of CH4 and CO gradually increased with the Rh loading increasing at temperatures lower than 400 °C, which is consistent with the conclusion of Fig. 2. This is because the rising reaction temperatures accelerate both CO2 methanation and reverse water–gas shift (RWGS) reactions for CO2 conversion. It is noteworthy that when operated temperatures exceeded approximately 415 °C, the partial pressure of CO initially increased while that of CH4 posed a gradual decline. Concurrently, the partial pressure of CO2 fell at slower rate for 1Rh–Al2O3 and 2Rh–Al2O3 samples, whereas H2 partial pressure started rising. This indicated that a side reaction occurred and resulted in hydrogen production at elevated temperatures. Combined with higher temperature conditions for hydrogen production and concentration changes of reactants, we infer that dry reforming of methane (DRM) side reactions occurred at temperatures higher than 415 °C.38 To verify the existence of DRM reaction at high temperature, we carried out the temperature-programmed surface reaction (TPSR) of DRM on 1Rh–Al2O3 (Fig. S5†). The generation of H2 and CO begins at ∼400 °C because of the strongly endothermic characteristic (ΔH = +247 kJ mol−1), which is in well line with DRM reaction occurring at ∼415 °C in our system. Combined with the actual CO2 conversion curve in Fig. 2, it is proposed that the decrease of CH4 concentration at high temperatures is mainly ascribed to the consuming of methane in dry reforming, rather than being limited by thermodynamic equilibrium.
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Fig. 3 The TPSR profiles of (a) 0.1Rh–Al2O3, (b) 0.5Rh–Al2O3, (c) 1Rh–Al2O3 and (d) 2Rh–Al2O3. The TPSR experimental conditions were the same as those for activity evaluation. |
Fig. 4a showed the CO-DRIFTS spectra of Rh–Al2O3 before reaction. Both peaks at ∼2087 and ∼2016 cm−1 can be observed in all the catalysts, which are attributed to the symmetric and asymmetric stretching vibrations of Rh(CO)2 adsorbed on Rh SAs, respectively.30,39 However, when the Rh loading exceeds 0.1 wt%, two distinct adsorption peaks emerge at approximately 1867 cm−1 and 2053 cm−1, ascribed to bridge and linear CO adsorption vibrations on Rh NPs, respectively.30,39 As the Rh loading increases, the CO adsorption signal on Rh NPs progressively intensifies, corresponding to the rise in a quantity of Rh NPs, which aligns with TEM image presented in Fig. 1. Fig. 4b showed the CO-DRIFTS spectra falling to room temperature after reaction at 400 °C. It can be seen that the various peaks appear at almost the same positions as peaks in the samples before reaction, indicating that the form of Rh remains unchanged in all the Rh–Al2O3 catalysts after the reaction. The redshift of the CO adsorption peak after the reaction mainly originates from the change in the electronic state of Rh (Δν ≈ 7 cm−1) such as the aggregation of Rh single atoms and instrumental errors or minor environmental fluctuations (Δν ≈ 5 cm−1), rather than from changes in the particle morphology.
Furthermore, the stability of four Rh–Al2O3 catalysts was studied through durability tests (Fig. S6†). The results show that the CO2 conversion rate of the 0.1Rh–Al2O3 catalyst drops to zero within one hour of the reaction, indicating that the isolated Rh single atom is unstable under the reaction conditions and deactivates rapidly. The CO2 conversion rate of the 0.5–2Rh–Al2O3 catalyst remained basically unchanged within 10 hours, demonstrating excellent long-term stability. The CO-DRIFTS spectra of the catalysts after the durability test showed that the 0.1Rh–Al2O3 catalyst exhibits bridging (1867 cm−1) and linear CO (2053 cm−1) adsorption vibrations on Rh NPs (Fig. S7†), which strongly indicates that isolated Rh single atoms agglomerate to form inactive aggregates under reaction conditions. This is consistent with the phenomenon reported in our previous work that single-atom catalysts are prone to sintering at high temperatures due to the weak stability of isolated metal sites.40,41 In contrast, the CO-DRIFTS spectra of the 0.5–2Rh–Al2O3 catalyst showed no significant changes compared with those before reaction, indicating that Rh nanoparticles in these samples were stable, which is in consistence with the durability test results.
The X-ray photoelectron spectra (XPS) of the Rh–Al2O3 catalyst before the reaction are shown in Fig. 5a–d. The negligible signal of Rh material observed on the 0.1Rh–Al2O3 catalyst in Fig. 5a can be attributed primarily to the low Rh content, which falls outside the detection range of XPS spectroscopy. The peaks with binding energies of ∼307.9 eV and ∼310.2 eV in the Rh 3d5/2 spectrum are attributed to Rh0 and Rh3+ species, respectively;42 with the Rh loading increases from 0.5% to 2%, the percentage of Rh0 also rises from 39% to 47%, as shown in Fig. 5b–d. It suggests a gradual increase of the particle size of Rh, which aligns with the findings from TEM analysis. Fig. 5e–h illustrates the Rh 3d XPS spectra after the 400 °C reaction, and we observe that the percentages of Rh0 in each catalyst after reaction have no obvious change compared to the corresponding catalysts before reaction, which is consistent with the findings in Fig. 4. The detailed results of XPS deconvolution of the Rh–Al2O3 catalyst are shown in Tables S1 and S2.†
The actual Rh loadings were further measured by ICP and are shown in Table 1, and it is seen that the values consequently approached the nominal Rh loading. The significant discrepancies in the stoichiometric ratios of CO adsorbed onto the surfaces of Rh SA and Rh NP, along with the variations in the ratios of CO adsorbed onto Rh NP surfaces with differing particle sizes,33 render traditional CO chemisorption techniques inadequate for precisely determining the dispersion of Rh–Al2O3 samples. In this study, the Rh SA content in other Rh–Al2O3 samples is semi-quantified based on the adsorption strength of Rh SA in the CO-DRIFT spectrum of each Rh–Al2O3 sample, with the 0.1Rh–Al2O3 sample serving as a reference point, and corresponding calculation process is outlined in Table S3 and Fig. S8.† The dispersion of Rh NP is derived from the mean particle size of Rh NP measured by TEM particle size statistics. Fig. 1 and S9† show representative TEM images of Rh NP, and the statistical mean size of Rh NP is listed in Table 1. The Rh NP dispersion was determined by calculating the reciprocal of the average size of Rh NP (in nm) and subsequently multiplying this value by a correction factor, following the methodology outlined by Zhang et al..43 Fig. S10† shows that the calculated Rh NP dispersion is consistent with the actual Rh NP dispersion when the correction coefficient is 0.3. Accordingly, the turnover frequency of CO2 conversion (TOFCO2) and CH4 generation (TOFCH4) as well as the theoretical turnover frequency of Rh NP CH4 generation (TOFCH4 of Rh NP) were calculated for the Rh–Al2O3 catalysts at 400 °C and detailed calculations are shown in Tables S4 and S5† As observed in Table 1, the minimal variation observed in the turnover frequency of CO2 (TOFCO2) across different Rh–Al2O3 samples indicates a comparable CO2 conversion efficiency between Rh single atoms (Rh SA) and Rh nanoparticles (Rh NP). Furthermore, the turnover frequency of CH4 (TOFCH4) for samples containing Rh loadings exceeding 0.5% is notably higher than that of samples with a Rh loading of 0.1%. This suggests that Rh NPs exhibit a superior capacity for CH4 generation compared to Rh SA. Additionally, the theoretical TOFCH4 of Rh NP was calculated and approximately three times the value of Rh SA (Table 1), suggesting better CO2 methanation activity of Rh sites on Rh NP than Rh SA. In this study, we conducted a comparative analysis of the turnover frequency values of CH4 generation (TOFCH4) calculated in this work with those in CO2 methanation using various Rh-based catalysts (Table S6†). The TOF values reported here are superior than others.
Sample | Rh actual contenta (wt%) | Rh SA contentb (wt%) | Rh NP content (wt%) | Mean size of Rhc NP (nm) | Rh NP dispersiond (%) | Rh total dispersione (%) | TOFCO2, netf (s−1) | gTOFCH4, net (s−1) | TOFCH4, net of Rhg NP (s−1) |
---|---|---|---|---|---|---|---|---|---|
a Measured by ICP-AES.b Determined by the IR intensity of CO adsorption on Rh single atom (SA), and the detailed calculation is shown in Table S3.c Determined by TEM image counts.d Rh NP dispersion = 1/mean size of Rh NP × 0.3.e Total dispersion = (Rh SA content × 100 + Rh NP content × Rh NP di2persion)/Rh actual content.f Net reaction rate of CO2, measured at 400 °C, and the detailed calculation is shown in Table S4.g Net CH4 formation rate, measured at 400 °C, and the detailed calculation is shown in Table S5. | |||||||||
0.1Rh–Al2O3 | 0.09 | 0.09 | — | — | — | 100 | 0.11 | 0.06 | — |
0.5Rh–Al2O3 | 0.46 | 0.17 | 0.29 | 0.7 | 42 | 64 | 0.13 | 0.10 | 0.16 |
1Rh–Al2O3 | 1.16 | 0.19 | 0.97 | 0.8 | 36 | 46 | 0.15 | 0.14 | 0.18 |
2Rh–Al2O3 | 1.81 | 0.22 | 1.59 | 1.2 | 25 | 34 | 0.14 | 0.13 | 0.17 |
We performed kinetic experiments on the CO2 methanation reaction on Rh–Al2O3, as shown in Fig. 6. From Fig. 6a, the apparent activation energy (Ea) gradually decreased with increasing Rh loading, indicating that Rh NP is more prone to catalyze CO2 methanation reaction. In Fig. 6b, the negative measured CO2 apparent reaction orders (nCO2) indicated that increasing partial pressure of CO2 for 0.1% Rh-loaded catalyst would inhibit the CH4 formation and conversely, partial pressure of CO2 could achieve the different degree of enhancement in the formation rate of CH4 for other samples, due to non-negative apparent reaction orders. In addition, the reaction orders of CO2 (nCO2) are approximately zero (−0.21–0.23), also indicating that CO2 adsorption and activation is not a significant influencing factor in the CO2 methanation reaction.
On the other hand, as shown in Fig. 6c, an increase in the partial pressure of H2 could significantly increase CH4 formation rates for all Rh–Al2O3 catalyst samples, because the H2 reaction orders (nH2) are greater than 0.80 and much higher than nCO2 (Fig. 6c), suggesting that H2 dissociation and activation should be key factors affecting catalytic performance of Rh–Al2O3 catalysts. In addition, the nH2 gradually decreases with increasing sizes of Rh particles and it also indicates that H2 adsorption becomes more pronounced for Rh nanoparticles with larger size, thus contributing to deep hydrogenation for the product CO or other intermediates, thereby indicating that high Rh loading favors methane generation. Subsequent density functional theory (DFT) calculations were employed to ascertain H2 adsorption strength on different supported Rh sites. The structural models of Rh1–Al2O3, Rh4–Al2O3, and Rh13–Al2O3 were used to represent Rh single atoms, Rh clusters, and Rh nanoparticles loaded on the Al2O3 surface, respectively40 and the calculated results and H2 adsorption structures are shown in Fig. 6d and Tables S7–9,† respectively. It can be found that the H2 adsorption becomes stronger for supported Rh catalysts with larger size, which is consistent with the experimental results of the reaction orders. The reaction orders of the reverse water–gas shift (RWGS) process are not determined because of low CO2 conversion rates of Rh–Al2O3 samples, with the exception of the 0.1Rh–Al2O3 samples (in Table S10†).
Table 2 shows the calculation results of mass and heat transfer criteria for CO2 hydrogenation reaction with different catalysts at 773.15 K. The average particle size of catalyst was measured by laser particle size analyzer (Fig. S11†). The relevant parameters to calculate mass and heat transfer limits of CO2 hydrogenation reaction was given in Tables S11 and S12.† The results show that both the mass transfer and heat transfer effects can be ignored under our experimental conditions.
Sample | T (K) | Deff (×10−6 m2 s−1) | kc (m s−1) | h (W m−2 K−1) | CWP (×10−3) | CM, mass (×10−3) | CM, heat (×10−6) |
---|---|---|---|---|---|---|---|
0.1Rh–Al2O3 | 773.15 | 8.09 | 1.15 | 580.04 | 1.32 | 0.132 | 3.73 |
0.5Rh–Al2O3 | 773.15 | 8.09 | 0.86 | 436.54 | 6.12 | 0.612 | 289 |
1Rh–Al2O3 | 773.15 | 8.09 | 0.84 | 426.82 | 7.19 | 0.719 | 400 |
2Rh–Al2O3 | 773.15 | 8.09 | 1.27 | 644.35 | 3.15 | 0.315 | 145 |
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Fig. 7 In situ DRIFTS spectra of (a) 0.1Rh–Al2O3, (b) 0.5Rh–Al2O3, (c) 1Rh–Al2O3 and (d) 2Rh–Al2O3 during CO2 hydrogenation at different temperatures. |
The peak appearing at ∼2000 cm−1 is attributed to the CO adsorption peak on Rh,20,34,50 and its appearance temperatures gradually fell with increasing Rh loadings, but the product temperature of CO gas increased with increasing Rh loadings, as shown in Fig. 3. The inconsistency suggested that the formed CO species should first be adsorbed on the surface sites and then released as gas CO via overcoming desorption barriers and the catalysts with higher Rh loading should pose the higher CO desorption barriers. Otherwise, it is found that the signal of CO (CO*) and gaseous CH4 appears at the same temperature and thus it is inferred that CO* is also a crucial intermediate species of methane generation.31,34,45,51 It is worth noting that at temperatures higher than 450 °C, the signals of gaseous CH4 and HCOO* disappeared, but the CO adsorption signal still existed, which further confirmed that DRM or RWGS reactions occur at high temperatures. The situation agrees with the conclusion that CO selectivity at high temperatures is enhanced as shown in Fig. 2.
To determine the change of each pathway to the formation of CH4, the intensity of the CO* (∼2000 cm−1) and m-HCOO* (1587 cm−1) bands were calculated by the adsorbing intensity of the highest point of the peak position minus the adsorbing intensity of the baseline in each IR spectrum. Intensity values were plotted in function of temperature for each sample, as shown in Fig. 8. It can be found that the intensities of both intermediates increase with the elevated temperatures until up to 250 °C or 300 °C for all samples. When the temperature exceeded that temperature, the intensity of HCOO* reversed to gradually decrease, illustrating the conversion of formate to the product CH4. However, the intensity of CO* started to increase again when the temperature high than 350 °C, attributing to the produced CO species of DRM reaction at high temperature. Accordingly, both pathways contributed to CO2 methanation reaction, the intensity of CO* increased at high temperature mainly attributed to DRM reaction, as evidenced by the TPSR results of mere DRM reaction (Fig. S5†).
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Fig. 8 In situ DRIFTS normalized band intensity versus temperature of CO* (∼2000 cm−1) and m-HCOO* (1587 cm−1). (a) 0.1Rh–Al2O3. (b) 0.5Rh–Al2O3. (c) 1Rh–Al2O3. (d) 2Rh–Al2O3. |
Experimental results from in situ infrared spectroscopy confirm that both formate and CO pathways coexist for Rh–Al2O3 catalyzing CO2 methanation regardless of Rh loading amounts and formate pathway is dominate for CO2 methanation when the temperature high than 400 °C. TOF calculation showed that TOFCO2 did not differ much between different Rh particle sizes, but TOFCH4 on Rh NP was three times higher than that of TOFCH4 on Rh SA, suggesting better CO2 methanation activity of Rh sites on Rh NP. Overall, the reaction orders of CO2 on Rh–Al2O3 catalyst are approximately 0, whereas nH2 approaches 1 and decreases with increasing Rh loading, suggesting that H2 dissociation and activation are critical factors influencing performance of Rh–Al2O3 catalysts. Additionally, H2 adsorbed more strongly on Rh catalysts with large particle size by DFT calculations. These results substantially enhance the systematic and thorough comprehension of the catalytic hydrogenation of CO2 over Rh–Al2O3 catalysts.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5ra03953c |
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