Alisha L.
Davidson
a,
Ramandeep S.
Dosanjh
a,
Stewart F.
Parker
ab and
David
Lennon
*a
aSchool of Chemistry, University of Glasgow, Joseph Black Building, Glasgow, G12 8QQ, UK. E-mail: David.Lennon@glasgow.ac.uk; Tel: +44(0)141 330 4372
bISIS Neutron and Muon Facility, STFC Rutherford Appleton Laboratory, Chilton, Didcot, Oxon OX11 0QX, UK
First published on 18th April 2025
The addition of CO2 to a syngas feed stream in Fischer–Tropsch to Olefin (FTO) catalysis is investigated by means of inelastic neutron scattering (INS) spectroscopy using ambient pressure CO hydrogenation at 623 K as a test reaction. The principal objective being to explore how the presence of CO2 affects the nature of a hydrocarbonaceous overlayer that forms during the conditioning phase of the catalytic process. The candidate FTO catalyst examined is Fe-based and doubly promoted with sodium (2000 ppm) and sulfur (100 ppm). Temperature-programmed oxidation profiles recorded after 3, 6, 12 and 24 h time-on-stream (T-o-S) reveal progressive carbon retention by the catalyst mainly in the form of amorphous carbon. The INS spectrum as a function of T-o-S confirms the presence of a hydrocarbonaceous overlayer, but with a much higher hydrogen concentration than previously observed for Fe-based FTO catalysts operating solely with a syngas feed. These preliminary results are considered with respect to a possible role for CO2 perturbing the equilibrium between iron carbides and oxides.
Sustainability spotlightCarbon dioxide is a greenhouse gas that is a major contributor to global warming and the climate crisis that the world is presently experiencing. Consequently, there is a major driver to develop chemical manufacturing processes that utilise CO2. The incorporation of CO2 as a feedstock in the emerging Fisher–Tropsch-to-olefins process, a route to produce valuable platform chemicals from biomass, is a candidate process for this role. The article examines fundamental aspects of the surface chemistry of the modified process operation, thereby improving the understanding of how the process could potentially contribute to a global warming mitigation strategy. The article connects with the following 8 UN SDG: 7, 9, 11, 12, 13, 15, 16 and 17. |
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Scheme 1 Overview of how under reaction conditions the hematite pre-catalyst is converted to an iron carbide phase that supports FTS chemistry. |
Whereas FTS has been extensively investigated by a wide variety of analytical techniques over many years, and despite hydrogen's pivotal role in the catalytic process, uncertainty remains as to how hydrogen is partitioned in the catalyst matrix as a function of reaction conditions. A technique well suited to investigating this conundrum is inelastic neutron scattering (INS), which can provide access to the vibrational spectrum of post-reaction catalyst samples, with special emphasis given to vibrations involving hydrogeneous modes. The topic of using neutron scattering techniques to interrogate heterogeneous catalysts has recently been comprehensively reviewed.10
Previous investigations employing inelastic neutron scattering (INS) to study iron-catalysed FTS, using ambient pressure CO hydrogenation as a test reaction, have enabled the vibrational spectrum of the catalyst to be obtained as a function of time-on-stream (T-o-S).4,5 In addition to the well-documented iron oxide → iron carbide transition (Scheme 1), the INS spectra reveal the additional formation of a hydrocarbonaceous overlayer,4,5,11–14 which is proposed to perform a ‘templating’ role in defining the active sites of the working catalyst.4
The water gas shift (WGS) reaction (eqn (1)) is also active over iron-based catalysts and is catalyzed by Fe3O4 that exists in dynamic equilibrium with carbides during FTS.15–19
CO + H2O ![]() | (1) |
The WGS reaction is close to equilibrium under high temperature operating conditions and the addition of CO2 to synthesis gas can therefore eliminate its production during FTS, improving carbon efficiency.20,21 However, as noted by Højlund-Nielsen and Bøgild-Hansen in their pioneering 1982 article, the introduction of CO2 into the feed stream can lead to conversion limitations in hydrocarbon synthesis.22 Adding further perspective to the role of CO2 in FTS chemistry, in 2021 Claeys and co-workers applied in situ magnetometer and X-ray diffraction techniques to investigate how CO2 could perturb reaction equilibria, highlighting the possibility of Hägg carbide oxidation,7 see Scheme 2. Against a background of increasing concerns over the role of atmospheric CO2 in global warming scenarios, and drivers for nudging chemical manufacturing processes to incorporate CO2 as a reagent (e.g. methanol production via CO2 hydrogenation),23 the inclusion of CO2 within a FTS platform represents a tantalising prospect.
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Scheme 2 An illustration indicating how CO2 can work against trends established within the iron-based catalyst conditioning process (Scheme 1), namely inducing the formation of magnetite from iron carbide, with the magnetite supporting WGS chemistry. Figure adapted with permission from M. Claeys, E. van Steen, T. Botha, R. Crous, A. Ferreira, A. Harilal, D. James Moodley, P. Moodley, E. du Plessis and J. L. Visagie, Oxidation of Hägg Carbide during High-Temperature Fischer–Tropsch Synthesis: Size-Dependent Thermodynamics and In situ Observations, ASC Catal., 2021, 11, 13866–13879. Copyright 2021 American Chemical Society.7 |
In recent times, the formation of long chain saturated hydrocarbons via FTS chemistry has been supplemented by a variant known as a Fischer–Tropsch to olefin (FTO) stage. Here, promotion of iron catalysts with an alkali metal and a small concentration of sulfur has been reported to shift the product slate away from long chain saturated hydrocarbons to short chain (C2–C4) olefins, key ‘platform chemicals’ that find wide application within the chemical industry.19,24–28 INS studies of FTO catalysts, again using the CO hydrogenation reaction as a test reaction, showed the hydrocarbonaceous overlayer to be similarly formed over the FTO catalysts, although the intensity of the sp2 hybridised C–H stretching mode was amplified relative to an unpromoted hematite sample.29,30 This modification of the hydrocarbonaceous overlayer was tentatively associated with a reduced hydrogen supply at the catalyst surface that favours olefinicity over saturated products.
Botes and co-workers report on the development of an olefin selective iron Fischer–Tropsch synthesis catalyst and utilise the addition of CO2 in the syngas feed stream during the reaction testing phase of their study.19Eqn (1) shows the introduction of CO2 into the syngas feed stream provides an opportunity to increase the CO available for reaction, whilst simultaneously reducing hydrogen availability; a scenario that could minimise C–C chain propagation and the formation of saturated products.
This article seeks to investigate how the addition of CO2 to a CO/H2 feed stream over a representative FTO catalyst, i.e. Fe–Na–S100,30,31 can affect the formation of the hydrocarbonaceous overlayer. To this end, ambient pressure CO hydrogenation at 623 K is again selected as the test reaction, as it allows examination of the Fe/CO/H2 surface chemistry without producing high molecular weight hydrocarbon products that would otherwise dominate the INS spectrum.12 The degree of CO2 incorporation adopted follows that outlined by Botes et al., who utilised a H2:
CO ratio of 4
:
1.19 Comparisons will be made to previous ambient pressure measurements made at 623 K using the more traditional H2
:
CO = 2
:
1 mixture8 over Fe–Na–S100 that are reported elsewhere.31
The product stream was analysed by an in-line mass spectrometer (Hiden Analytical, HPR20 QMS Sampling System). Once the specific reaction was complete, the reactant gases were stopped, and the sample cooled to room temperature under the helium carrier gas. The reactor cell was isolated and placed in an argon-filled glove box (MBraun UniLab MB-20-G, [H2O] < 1 ppm, [O2] < 2 ppm) before the sample was loaded into an aluminium sample holder and sealed via an indium wire gasket.32 All INS measurements were performed using the MAPS direct geometry spectrometer10 at the ISIS Neutron and Muon Facility (Chilton, UK).33 Spectra were recorded at 20 K with incident neutron energies of 650 meV and 250 meV using the A-chopper package. Quantification of the ν(C–H) feature observed by INS was achieved following a calibration protocol described elsewhere.4,5,29–31,34
Ex situ temperature programmed oxidation (TPO) measurements were performed on 10 mg of post-reaction samples using a micro-reactor test line composed of ⅛ in. diameter stainless steel tubing, a description of which can be found elsewhere.4,14 The CO2 peak area was quantified by measuring the CO2 response from the in situ TPO of known masses of graphite (Sigma-Aldrich, 99.9%).35 The catalyst was loaded into a ¼ in. quartz tube reactor and plugged with quartz wool. The reactor was housed within a tube furnace (Carbolite MTF 10/15/30) equipped with PID control. All gas flows were monitored using an in-line quadruple mass spectrometer (Hiden Analytical, HPR-20) attached to the reactor exit line via a differentially pumped, heated quartz capillary. Oxygen (5% in He, 75 sccm, BOC Ltd, 99.5%) was introduced to the sample and the reactor heated to 1173 K at 5 K min−1 using the mass spectrometer to monitor the eluting gases.
Sample | FT [μmol g−1 s−1] | CH4 (%) | CO2 (%) | C2–C4 (%) | C5+ (%) | C2 olefin![]() ![]() |
C3 olefin![]() ![]() |
C4 olefin![]() ![]() |
---|---|---|---|---|---|---|---|---|
Fe-ref | 78.5 ± 3.9 | 24.9 ± 1.2 | 26.2 ± 1.3 | 41.8 ± 2.1 | 33.3 ± 1.7 | 0.1 ± 0.01 | 0.8 ± 0.04 | 1.3 ± 0.1 |
Fe–Na–S100 | 47.9 ± 2.4 | 9 ± 0.5 | 33.6 ± 1.7 | 34.2 ± 1.7 | 56.8 ± 2.8 | 8.1 ± 0.4 | 8.7 ± 0.5 | 7.8 ± 0.4 |
In this study, Fe–Na–S100 was exposed to ambient pressure CO hydrogenation conditions at 623 K with the inclusion of a CO2 co-feed, for 3, 6, 12 and 24 h, with a representative profile shown in Fig. 1a. This is directly compared in Fig. 1b to the same catalyst, Fe–Na–S100, exposed to ambient-pressure CO hydrogenation conditions without a CO2 feed in the same reactor, as reported in a previous study.31 Whereas previous studies using a micro-reactor arrangement revealed a three-stage conditioning process that involved the transitions indicated in Scheme 1,4,5,14Fig. 1 is better described by a two-stage process: the initial reduction step requires approximately 2 h T-o-S; thereafter, the system exhibits pseudo-steady state operation. This scenario applies both to Fig. 1a and b. It is possible that the larger Inconel reactor is causing a reduction in profile resolution compared to the micro-reactor studies.
Fig. 1a shows the inclusion of CO2 into the feedstream leads to more stable methane production on completion of the reduction stage compared to its absence (Fig. 1b). The water production is also more stable. Thus, the CO2 appears to have induced changes to the reaction profile but only to a modest degree. No C2–C4 olefins or higher hydrocarbons were observed for these ambient pressure measurements conducted in the INS Inconel reactor. As noted in the Introduction, the reaction conditions used by Botes et al.19 means that the hydrogen ratio used in the two runs presented in Fig. 1 is higher for the CO2 co-feed case, a situation that potentially compromises direct comparisons between the two runs.
Fig. 2 presents the ex situ post-reaction temperature-programmed oxidation (TPO) profiles after 3, 6, 12 and 24 h of reaction, showing CO2 production that signifies carbon retention by the catalyst. Fig. 3 displays the oxygen consumption profiles alongside the individual TPO plots, confirming that the provision of the oxidant was sufficient in all cases. Previous studies have identified and quantified three distinct carbonaceous components: α – reactive carbon, β – amorphous carbon and γ – iron carbides/polyaromatic carbonaceous species.4,5,30,31Fig. 4 compares the TPO profiles for the Fe–Na–S100 catalyst after 12 h reaction (ambient pressure CO hydrogenation at 623 K) in the absence (red) and presence (blue) of a CO2 co-feed. Whilst the α, β and γ features are observable when CO2 is absent, peak resolution is degraded when CO2 is present, and the profile is dominated by an intense feature exhibiting a peak maximum in the range 650–680 K. On the basis of the Tmax value, the desorption feature is assigned to amorphous carbon.31 It is surmised that the larger amounts of carbon laydown observed in the presence of the CO2 co-feed (Fig. 4) are responsible for the lower resolution TPO profiles.
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Fig. 2 Ex situ temperature-programmed oxidation profiles for Fe–Na–S100 after exposure to CO hydrogenation conditions with a CO2 co-feed at 623 K for 3, 6, 12 and 24 h T-o-S. |
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Fig. 3 TPO profiles (pink) for T-o-S = (a) 3, (b) 6, (c) 12 and (d) 24 h, with the figures including the associated oxygen consumption profiles (black). |
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Fig. 4 Ex situ temperature-programmed oxidation profiles for Fe–Na–S100 after exposure to CO hydrogenation conditions with (blue) and without (red) a CO2 co-feed at 623 K for 24 h T-o-S. The ‘without CO2’ profile has been reported previously by Davidson et al.31 and is included in this figure for comparison purposes. |
Fig. 5 correlates the extent of total carbon retention as a function of T-o-S for reactions undertaken in the presence of CO2. The total quantity of carbon retention after 24 h T-o-S is 430 mmolC gFe−1. This value significantly exceeds that reported for an unpromoted hematite Fischer–Tropsch synthesis catalyst operating solely with a 2:
1 syngas feed (24 h T-o-S = 27 mmolC gFe−1)31 by a factor of >16. Moreover, the overall profile can be deconvoluted into two kinetic regimes: the period 0–12 h T-o-S corresponds to a carbon deposition rate of 5.0 mmolC gFe−1 h−1, whilst the period 12–24 h corresponds to a retention rate of 32.5 mmolC gFe−1 h−1, i.e. 6.5 times that observed for the lower runtimes.
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Fig. 5 (a) Carbon content (mmolC gFe−1) observed from the ex situ TPO profiles of samples exposed to CO hydrogenation conditions with a CO2 co-feed for 3, 6, 12 and 24 h. |
Lastly for this section, it is noted that on transferring the 24 h reacted sample from the large-scale Inconel reactor to the aluminium INS sample holder in the glove box, large quantities of carbon were clearly observed. The visual extent of this carbon formation exceeded anything previously seen for this campaign of INS investigations of FTS and FTO catalysis.4,5,11–14,29–32
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Fig. 6 The left-hand frames present INS spectra for the Fe-based doubly promoted Fischer–Tropsch catalyst (Fe–Na–S100) after CO hydrogenation with a CO2 co-feed at 623 K for 0–24 h (red, blue, brown and orange) with incident energies of (a) 650 meV and (c) 250 meV. The right-hand frames present INS spectra for the Fe-based doubly promoted Fischer–Tropsch catalyst (Fe–Na–S100) after CO hydrogenation performed in the absence of a CO2 co-feed at 623 K for 24 h (green) with incident energies of (b) 650 meV and (d) 250 meV. The spectra presented in (b) and (d) have been reported previously by Davidson et al.31 and are included in this figure for comparison purposes. |
For the CO2 included dataset, inspection of the stretching region (2400–3750 cm−1) presented in Fig. 6a identifies the presence of hydrocarbon moieties, with a prominent sp2 hybridised carbon ν(C–H) feature at 3048 cm−1 and a sp3 hybridised carbon ν(C–H) shoulder at 2932 cm−1 observed for all samples.4,29–31 The deformation region of the spectra (400–1600 cm−1) (Fig. 6c), highlights various bands that have been observed previously.4,5,11–13,29–32 These can be summarised as follows: C–C torsion mode of edge carbon atoms contained within a polycyclic aromatic network (506 cm−1); out-of-plane C–H deformation of either an olefinic or aromatic group (871 cm−1); alkenic δ(C–H) (953 cm−1); CC–H in plane deformation of a polyaromatic hydrocarbon (1160 cm−1) and methyl deformation modes (1389, 1451 cm−1).30 Overall, with the inclusion of the CO2 co-feed, the INS spectrum for the FTO catalyst by 24 h T-o-S (Fig. 6a and c) is comparable to that previously reported for Fe–Na–S100 under standard CO hydrogenation conditions (Fig. 6b and d).31 This coincidence in the overall spectral profile signifies that, despite the alteration to the feed stream, the nature of the hydrocarbonaceous overlayer is effectively unchanged.
However, other aspects of the INS spectrum are noticeably different. Specifically, for Fe–Na–S100 in the absence of CO2 it is reported that a band at 591 cm−1, assigned to the A1g phonon of magnetite (Fe3O4) and indicative of an under reduced catalyst, is only prominently observable up to 3 h on stream.31 Notably, this band is only weakly observed in Fig. 6d. In contrast, Fig. 6c shows this feature to be retained throughout the full 24 h period. Following the lead of Højund-Nielsen and Bøgild-Hansen,22 and with reference to the equilibrium condition depicted in Scheme 2, a possible explanation is that the presence of CO2 prevents complete reduction of magnetite to Hägg carbide; either at the surface, in the bulk, or indeed both. This effect of CO2 co-feeding has also been observed recently in similar studies of fused iron catalysts.16
On employing previously established calibration procedures,4,5,10–14,29–31 the hydrogen concentration of the ν(C–H) modes observed in Fig. 6a can be quantified and are presented in Fig. 7. Both the aliphatic (2932 cm−1) and aromatic/olefinic (3048 cm−1) components of the hydrocarbonaceous overlayer in the presence of CO2 show comparable profiles, increasing steadily to 12 h on stream before exhibiting a dramatic change in formation rate. For the period 0–12 h T-o-S the sp2 hybridised carbon ν(C–H) feature at 3048 cm−1 signifies a formation rate of 2.3 μmolH gFe−1 h−1, whilst for the period 12–24 h this rises to a value of 7.4 μmolH gFe−1 h−1, corresponding to an increase of × 3.2. At T-o-S = 24 h, the sp3 and sp2 hybridised ν(C–H) components respectively correspond to 23 and 116 μmolH gFe−1. This sudden increase in INS intensity, signifying an increase in retained hydrogen, is unprecedented. For example, Fig. 7 additionally presents the hydrogen retention values for the sp3 and sp2 hybridised ν(C–H) components of Fe–Na–S100 determined in the absence of a CO2 co-feed (dashed lines).31 These values (3.7 and 9.6 μmolH gFe−1 respectively) are an order of magnitude below that seen in the presence of the CO2 co-feed.
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Fig. 7 Hydrogen concentration (μmol gFe−1) of sp3 hybridised carbon feature at 2932 cm−1 (hollow) and sp2 hybridised carbon feature at 3048 cm−1 (solid) identified in Fig. 6(a) of Fe–Na–S100 in the presence of CO2 (solid lines), and in the absence of CO2 (dashed lines). |
3Fe5C2 + 26H2O → 5Fe3O4 + 6CO + 26H2 | (2) |
3Fe5C2 + 26CO2 → 5Fe3O4 + 32CO | (3) |
Fig. 1 indicates continuous CO and H2 turnover that is maintained with the addition of CO2 to the syngas feedstream. The observation of magnetite in the INS spectra is attributed to the presence of CO2 retarding bulk carbide formation during activation rather than preventing complete surface reduction or causing re-oxidation at the onset of catalyst turnover.
The temporal profiles of the TPO plots and the INS intensities hint at coordinated events occurring at the catalyst surface. Concentrating firstly on the carbon, Fig. 5 shows the formation of amorphous carbon signal to dramatically increases at T-o-S = 12 h. Specifically, a 6.5-fold increase in the carbon deposition rate is observed for the period 12–24 h compared to that consistently observed in the first 12 h period. Poignantly, Fig. 7 shows this reaction time coincides with a significant increase in the concentration of the hydrocarbonaceous overlayer, as signified by the intensity of the sp2 hybridised carbon ν(C–H) feature at 3048 cm−1, which exhibits a 3.2-fold increase for the latter 12 h period of T-o-S compared to that observed during the initial 12 h block. Within the complexity of the iron catalyst's conditioning phase (Scheme 1), we propose that the level of CO2 inclusion and operating conditions used here can progressively modify the chemical potential of the surface. The precise way this occurs is uncertain. Indeed, in a way, the TPO and INS trends are contradictory: the extensive carbon formation hints at hydrogen-lean conditions (which would favour olefin formation), whilst the enhanced incorporation of hydrogen into the hydrocarbonaceous overlayer seemingly goes against this trend.
The relative rates of enhancement observed for periods exceeding 12 h T-o-S are informative concerning a possible inter-play between carbon retention and a hydrocarbonaceous overlayer. In their examination of the temporal behaviour of an unpromoted FTS catalyst applied to ambient pressure CO hydrogenation at 623 K, Warringham and co-workers proposed a reaction model where amorphous carbon formation and a hydrocarbonaceous overlayer were individual components of a conditioned catalyst.14 Whilst a consideration of a synchronised increase in the rate of amorphous carbon build-up and enhanced formation of the sp2 hybridised carbon ν(C–H) mode, as signified in, respectively, Fig. 5 and 7, may suggest that the carbon and hydrogen retention processes are inherently linked, inspection of their relative formation rates suggests otherwise. Rather, it is thought that following a catalyst conditioning stage of 12 h duration, the greater acceleration of carbon retention over that of generation of hydrocarbonaceous species (carbon accumulation is approximately twice that of hydrogen retention) is indicative of distinct processes taking place, as invoked within Warringham and co-workers’ reaction model.14 Concerning the substantial quantities of amorphous carbon being produced, this could be due to the Boudouard reaction (eqn (4)).
2CO ![]() | (4) |
• In comparison to operation in the absence of CO2, the reaction profile exhibits increased and sustained methane production (Fig. 1).
• The presence of CO2 leads to a substantial increase in the formation of amorphous carbon. After 24 h T-o-S this corresponds to 430 mmolC gFe−1 (Fig. 5), a value 16 times greater than that observed in the absence of CO2.
• The presence of CO2 in the syngas feedstream appears to have no significant effect on the form of a hydrocarbonaceous overlayer, the spectra exhibiting a comparable spectral profile to that observed for FTS and FTO catalysts (Fig. 6).
• The degree of hydrogen incorporation within the hydrocarbonaceous overlayer is considerably increased in the presence of a CO2 co-feed (Fig. 7). For example, after 24 h T-o-S the sp2 hybridised ν(C–H) component corresponds to 116 μmolH gFe−1, compared to a value of 9.6 μmolH gFe−1 in the absence of CO2, a 12-fold enhancement.
• A coincidence of increased rates of carbon (Fig. 5) and hydrogen (Fig. 7) retention into the catalyst matrix is observed at 12 h T-o-S. Given the approximately two-fold disparity in retention rate enhancement for carbon compared to hydrogen, these are thought to represent distinct chemical pathways.
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