B.
Venezia‡
a,
E.
Cao‡
a,
S. K.
Matam
bc,
C.
Waldron
a,
G.
Cibin
d,
E. K.
Gibson
be,
S.
Golunski
c,
P. P.
Wells
bf,
I.
Silverwood
g,
C. R. A.
Catlow
bch,
G.
Sankar
h and
A.
Gavriilidis
*a
aDepartment of Chemical Engineering, University College London, London WC1E 7JE, UK. E-mail: a.gavriilidis@ucl.ac.uk
bThe UK Catalysis Hub, Research Complex at Harwell, Harwell, OX11 0FA, UK
cCardiff Catalysis Institute, School of Chemistry, Cardiff University, Cardiff CF10 3AT, UK
dDiamond Light Source Ltd., Harwell Science and Innovation Campus, Didcot OX11 0DE, UK
eSchool of Chemistry, The University of Glasgow, Glasgow G12 8QQ, UK
fSchool of Chemistry, University of Southampton, Southampton SO17 1BJ, UK
gISIS Pulsed Neutron and Muon Facility, Science and Technology Facilities Council, Rutherford Appleton Laboratory, Harwell Science and Innovation Campus, Oxon, UK
hDepartment of Chemistry, University College London, London WC1H 0AJ, UK
First published on 16th October 2020
Operando X-ray absorption spectroscopy (XAS), diffuse reflectance infrared Fourier transform spectroscopy (DRIFTS) and mass spectrometry (MS) provide complementary information on the catalyst structure, surface reaction mechanisms and activity relationships. The powerful combination of the techniques has been the driving force to design and engineer suitable spectroscopic operando reactors that can mitigate limitations inherent to conventional reaction cells and facilitate experiments under kinetic regimes. Microreactors have recently emerged as effective spectroscopic operando cells due to their plug-flow type operation with no dead volume and negligible mass and heat transfer resistances. Here we present a novel microfabricated reactor that can be used for both operando XAS and DRIFTS studies. The reactor has a glass–silicon–glass sandwich-like structure with a reaction channel (3000 μm × 600 μm; width × depth) packed with a catalyst bed (ca. 25 mg) and placed sideways to the X-ray beam, while the infrared beam illuminates the catalyst bed from the top. The outlet of the reactor is connected to MS for continuous monitoring of the reactor effluent. The feasibility of the microreactor is demonstrated by conducting two reactions: i) combustion of methane over 2 wt% Pd/Al2O3 studied by operando XAS at the Pd K-edge and ii) CO oxidation over 1 wt% Pt/Al2O3 catalyst studied by operando DRIFTS. The former shows that palladium is in an oxidised state at all studied temperatures, 250, 300, 350, 400 °C and the latter shows the presence of linearly adsorbed CO on the platinum surface. Furthermore, temperature-resolved reduction of palladium catalyst with methane and CO oxidation over platinum catalyst are also studied. Based on these results, the catalyst structure and surface reaction dynamics are discussed, which demonstrate not only the applicability and versatility of the microreactor for combined operando XAS and DRIFTS studies, but also illustrate the unique advantages of the microreactor for high space velocity and transient response experiments.
In the last two decades, there has been a surge in the application of operando techniques.19–23 However, operando cells often suffer from a range of issues including poor sealing, contamination, large dead volume, and temperature and concentration gradients along the catalyst bed, which can lead to biased conclusions.19,24,25 Furthermore, in order to reduce mass transfer resistances across the catalyst bed and to derive reliable intrinsic kinetic data, the operando cells must be capable of handling high space velocities.26,27 Different configurations of operando and in situ reactor cells have been reported.28–34 Among these, it is common to find modified Harrick cells, which have been used for combined DRIFTS and XAS studies.32–34 However, these cells have a large dead volume that can lead to a broad residence time distribution, by-pass and inhomogeneous reaction conditions. Agostini et al. proposed a spectroscopic cell with a body-dome configuration, which was optimised for time-resolved combined XAS/DRIFTS/MS studies.35 This consisted of a body containing the sample holder and the heater, and a dome including the X-ray and IR windows. The catalyst in powder form was hosted in a crucible, placed in between two carbon-glass windows transparent to X-rays and below a CaF2 window for IR radiation. The reactor could be operated at up to 600 °C and 5 bar. The dead volume in the reaction chamber was around 0.5 cm3 which increased to 1 cm3 when a dome for higher pressure experiments had to be employed. In other studies, different configurations were reported as alternatives.27,36,37 Among these, Chiarello et al. demonstrated a spectroscopic cell for in situ transmission XAS with DRIFTS.36 In this design, the X-ray and IR beams were focussed on the same optical window and were perpendicular to the catalyst bed. Furthermore, the gas inlet and the outlet shared the same direction and the dead volume was reduced compared to a modified Harrick33 or SpectraTech cell.38 However, the gas flow was replaced in the cell in 5 s, due to the dead volume of the inlet and outlet tubes and for combined IR-XAS studies the authors had to drill a hole in the CaF2 window for IR and fill it with carbon based glue to allow X-ray passing through. Dann et al., developed a new spectroscopic packed-bed reactor to study the kinetic oscillations of CO oxidation over a Pd/Al2O3 catalyst with combined energy dispersive EXAFS (EDE) and DRIFTS.37 The reactor cell was made of pure aluminium with a square cross sectional channel (5 mm × 5 mm) that hosted the catalyst in the form of pellets (250–335 μm). It had thin walls on two opposite sides, to allow X-ray spectroscopy analysis to be performed in transmission mode, while on top a rectangular CaF2 window was installed for IR transmission. The heating plate was placed underneath the reactor and the temperature was measured near the outlet region. This cell was tested up to 140 °C and allowed to perform simultaneous operando EDE/DRIFTS at 8 different positions along the packed bed.
The use of microfluidic and microfabricated reactors which can offer accurate control of process conditions, homogeneous temperature distribution and a distinct flow pattern, has been reported for operando spectroscopic studies under realistic reaction conditions.39–47 Such microreactors are valuable and compact tools for spectroscopic studies24,39 including Raman,40,48,49 IR,50–53 X-ray diffraction (XRD)45,54,55 and XAS.42,45,55,56 Among such reactors, silicon microfabricated reactors have unique advantages due to their high thermal conductivity, chemical inertness and mechanical stability. Micromachining allows fabricating microreactors with accurate and versatile microchannel geometries. Silicon microreactors, sealed with glass through an anodic bonding process, can be operated up to 500 °C. In particular, the transparency of silicon to X-rays and IR beams (also glass for Raman) makes the glass-bonded silicon microreactor ideal for combined operando XAS and DRIFTS studies.55 In our previous work, a silver sputter-coated microchannel of a silicon-glass microreactor was employed for operando Raman spectroscopic studies of continuous oxidative dehydrogenation of methanol to formaldehyde.40 The silver sputter-coated microchannel of the microreactor served itself as a catalyst surface and it enabled us to evaluate the effect of temperature and reaction feed composition on the catalyst structure and activity, and to identify reaction intermediates. The same reactor was also employed for in situ XAS studies at the silver K-edge in fluorescence mode.42 This work demonstrated the applicability and versatility of the microchannel reactor for multi technique operando spectroscopic studies. However, the application of the sputter coated microchannel reactor is limited to unsupported metal catalysts. Therefore, here we report a novel silicon–glass microreactor for supported catalysts that can be used for both operando XAS and DRIFTS, addressing many of the limitations imposed by conventional operando cells. The applicability and versatility of the microreactor are demonstrated by investigating the Pd K-edge during methane combustion over 2 wt% Pd/Al2O3 and surface adsorbed species during carbon monoxide oxidation on 1 wt% Pt/Al2O3. The experiments provide new information on catalyst structure and dynamics for these widely studied systems.
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Fig. 1 Technical drawing of the silicon microreactor. Back side (left), front side (right). Dimensions are in millimetres. |
The microfabrication process was performed via double-sided photolithography (Q4000-6, Quintel) followed by deep reactive-ion etching (DRIE, STS ASE) of each side of a double-sided polished 1 mm thick and 100 mm diameter silicon wafer (undoped float zone grown, CRYSTRAN UK). For the wafer, three microfabrication steps were carried out. The front side of the reactor with its gas channel was processed first, patterned and etched to ca. 200 μm. Except for the inlet/outlet holes, the etched channel was then covered with a photoresist (SPR-220-7, Rohm and Haas) which was applied manually using a small pipette tip. This was followed by a soft baking at 90 °C for 10 min. The front side was further etched by ca. 200 μm for the holes. Afterwards, the wafer with the processed front side was cleaned thoroughly with Piranha solution (H2SO4:
H2O2 = 3
:
1) at 100 °C for 15 min, followed by another lithography step. The back side of the wafer was patterned with the help of infrared beam alignment. Subsequently, DRIE was used to etch for 600 μm to create the reactor channel. The holes on the silicon layer were etched through to form connections between the gas inlet channel and the reaction channel. The micro-fabricated silicon wafer was then cut into three individual reactor chips. Double-sided anodic bonding followed to seal the two sides of the silicon layer with the two glass layers by performing two steps of anodic bonding. The first step was to assemble the front glass layer to the front surface of the silicon layer on a hotplate (Stuart SD162) at a temperature of 420 °C while applying a DC voltage of 500 V across the assembly (cathode attached to the silicon and anode to the glass). After the first anodic bonding, the assembled silicon–glass chip was removed from the hot plate, cooled down and cleaned with Piranha solution. The second step was performed by placing the silicon–glass chip onto the hotplate (when the hot plate was cool enough) with the back surface of the silicon layer facing up and then putting the back glass cover on the top of the silicon chip by aligning the holes on the glass cover to the inlet and outlet holes on the silicon layer. After heating the hotplate to 420 °C, a DC voltage of 500–700 V was applied across the sandwich assembly.
The microreactor was incorporated in an in-house made heating unit (see ESI†). The heating was achieved using a ceramic heater (25 mm × 50 mm × 2.5 mm, ULTRAMIC® ceramic heaters, Watlow) which was fitted into a stainless steel holder. High temperature O-rings (Perlast G80A, O Rings Ltd) were used to seal the inlet and outlet connections to the microreactor, which was placed onto the heater holder and fixed firmly in position using the top clamp of the holder. The microreactor can be operated up to a maximum temperature of 400 °C due to the material used for insulating the electrical connections of the thermocouple embedded in the ceramic heater, which can be changed to achieve a higher reaction temperature if required.
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Fig. 3 Microreactor assembly (a) at the beamline B18 at the Diamond Light Source for the operando XAS/MS study and (b) at the Research Complex at Harwell for the operando DRIFTS/MS study. |
Operando XAS studies were conducted similarly to the reaction test in section 2.2. The 2 wt% Pd/Al2O3 catalyst particles (27.7 mg of 53–63 μm sieve fraction) were loaded into the microreactor. The catalyst was heated up at 10 °C min−1 under 10% O2/He flow and calcined at 400 °C for 30 min. The temperature was then decreased to 250 °C and the gas flow was switched from 10% O2/He to 1% CH4, 4% O2 and 5% Ar in He (total flow rate of 40 NmL min−1). The combustion reaction was carried out at 250, 300, 350 and 400 °C (at 10 °C min−1) with a dwell time of around 45 min at each temperature to achieve steady state conditions. Under steady state, the catalyst bed at the inlet region was probed with the X-ray beam in transmission mode.
In another experiment, a temperature-resolved reduction of 2 wt% Pd/Al2O3 was performed with methane in flow. After calcination at 400 °C, the catalyst was cooled down to 225 °C under 10% O2/He flow. Then the gas mixture was switched from 10% O2/He to 1% CH4/He at 40 NmL min−1 and the temperature of the reactor was gradually increased from 225 to 300 °C at a rate of 1 °C min−1 while monitoring the catalyst at the bed inlet by XAS. After the experiment, the gas mixture was switched back to 10% O2/He, the temperature increased up to 400 °C and the catalyst was re-calcined. This time the X-ray beam was directed at the outlet bed position and a temperature-resolved reduction was performed again under 1% CH4/He at 40 NmL min−1 from 225 to 305 °C (1 °C min−1). During the two temperature-resolved reductions, XAS scans were taken every 3.46 min, generating 21 and 24 spectra respectively.
The raw XAS spectra were processed using the software Athena.59 The X-ray absorption near edge structure (XANES) spectra were pre-edge subtracted and normalised to the post-edge background. The linear combination fitting (LCF) of the normalised XANES spectra was then performed around the Pd K-edge, 24150–24
986 eV, using the software Athena.59 The XANES spectra of the reference Pd metal foil were used as standard for the palladium metal (Pd0) in the LCF, while for the PdO component the spectra at the inlet during calcination were taken as reference. Their weightings were constrained to be between 0 and 1 and their sum to be equal to 1. The fitting quality was assessed using R-factors, which were consistently low for all the fittings (R-factor = 0.00083 ± 0.00021). An example of a LCF of a XANES spectrum for the catalyst at 250 °C is presented in Fig. S4 (see ESI†). The Fourier transform (FT) of the EXAFS data was performed on the k3-weighted functions between 2.7 and 10 Å−1.
Oxidation of carbon monoxide was performed using a typical amount of 29.6 mg (sieve fraction of 38–53 μm) of a commercial 1 wt% Pt/Al2O3 catalyst (Sigma Aldrich). The catalyst was heated up at 10 °C min−1 under 10% O2/He flow and calcined at 400 °C for 60 min. Then the flow was switched from 10% O2/He to pure He, and then to 10% H2/He at 400 °C for 30 min in order to reduce the catalyst. Subsequently, the hydrogen flow was replaced with pure helium at the same temperature to flush the catalyst bed for 15 min and the reactor was cooled to 30 °C under the same helium flow. Temperature-resolved CO oxidation over the reduced Pt/Al2O3 catalyst was then conducted between 30 and 400 °C using 10% O2/He (at 30 NmL min−1) and 10% CO/He (at 10 NmL min−1) reaction mixture. The reaction temperature was ramped at 5 °C/min from 30 to 400 °C and DRIFTS spectra were collected approximately every 30 s, while reaction products were simultaneously monitored by MS. At 400 °C, the reaction mixture was switched to 10% O2/He for 30 min to calcine the catalyst. Afterwards, the catalyst was cooled to 30 °C (10 °C min−1) under the same O2/He flow. A temperature-resolved CO oxidation over the oxidised 1 wt% Pt/Al2O3 catalyst was carried out using the same reaction mixture and temperature ramp as described above for the CO oxidation with the pre-reduced catalyst.
After the reaction at 400 °C, the temperature of the reactor was decreased to 310 °C and the gas was switched to a stoichiometric composition of 10% O2/He (5 NmL min−1), 10% CO/He (10 NmL min−1), balance He (25 NmL min−1) to study possible concentration gradients of adsorbed species along the catalyst bed by DRIFTS. For this experiment, the catalyst bed was probed under steady-state conditions with DRIFTS from the inlet to the outlet of the catalyst bed, by moving (at 2 mm steps) the reactor stage.
All experiments were conducted using an Agilent Cary 680 series spectrometer equipped with a Harrick DaVinci arm (see Fig. 3). The DaVinci arm was fitted with Praying Mantis optics, which focussed the IR beam onto the catalyst bed of the microreactor. The microreactor outlet was connected to a Hiden QGA mass spectrometer for analysis of the reactor effluent. As in the operando XAS experiments, the microreactor was placed onto an adjustable stage that was located under the DaVinci arm. The experimental rig schematic is shown in the ESI.† The extended IR focal length of the Praying Mantis optics allowed the microreactor to be located at about 4.7 mm below the DaVinci arm. Prior to DRIFTS experiments, alignment of the IR beam along the central line of the catalyst bed was required. DRIFTS spectra were acquired by taking 64 scans with a resolution of 4 cm−1 using a liquid nitrogen cooled mercury cadmium telluride (MCT) detector.
In all the experiments, the catalyst performance was assessed using the reactant consumption rate, r, according to eqn (1), where F is the inlet molar flowrate, yin and yout are the gas inlet and outlet concentrations (vol%, methane or carbon monoxide) respectively and ncat is the molar amount of metal catalyst.
![]() | (1) |
![]() | (2) |
Reference | wt% Pd | Catalyst pretreatment | y in,CH4, % | O2/CH4, − | r CH4, molCH4 molPd−1 h−1 |
---|---|---|---|---|---|
Burch et al.60 | 4 | Calcination | 0.8 | 20 | 91 |
Briot et al.61 | 1.95 | Reduction | 1 | 4 | 10 |
Briot et al.61 | 1.95 | Ageing | 1 | 4 | 65 |
Burch et al.62 | 4 | Calcination | 0.3 | 5 | 35 |
Mouaddib et al.63 | 1.93 | Reduction | 1 | 4 | 5 |
Mouaddib et al.63 | 1.93 | Ageing | 1 | 4 | 70 |
This work | 2 | Calcination | 1 | 4 | 107 |
Fig. 5 shows the temperature values along the reactor bed during methane combustion. It is evident that no large temperature gradient is present along the glass beads and the catalyst bed, especially below 400 °C. At 400 °C, the temperature profile along the bed shows the highest variation (±1 °C from the set temperature). Based on the conversion and temperature profiles obtained, the microreactor design and performance was judged to be satisfactory to be employed for operando XAS/MS studies for the combustion of methane.
From the observed reaction rate (107 molCH4 molPd−1 h−1), the catalyst particle size (53–63 μm sieve fraction) and the gas physical properties at 400 °C, the Péclet (Pe), Mears (MR) and Weisz–Prater (CWP) numbers can be calculated (see Table 2). The large Péclet number suggests that axial dispersion within the packed bed can be neglected, hence the microreactor can be regarded as an ideal plug-flow reactor. The low Mears and Weisz–Prater numbers indicate that the reactor operates under no external or internal mass transfer resistances, respectively. The details on the calculation of these numbers are reported in the ESI.†
Pe | MR | C WP |
---|---|---|
61 (>6) | 0.07 (<0.15) | 0.003 (≪1) |
In agreement with XANES and LCF data (Fig. 6(c) and (d)), the Fourier transform (FT) of the corresponding EXAFS data shows a contribution from oxygen in the first coordination shell of the PdO like structure at ca. 1.5 Å (phase shift uncorrected) and another contribution from the corresponding Pd–Pd pair in the second coordination shell at around 3 Å (see Fig. 7). No other peaks attributable to metallic palladium are apparent except for a small contribution from Pd–Pd metal (ca. 2.4 Å) at 250 °C. These results further indicate that the palladium was predominantly in oxidised state in the catalyst during reaction at all studied temperatures.
The stacked XANES, PdO and Pd metal component extracted from LCF analysis of XANES data and the FT of the EXAFS data collected for the catalyst at the reactor inlet are plotted as function of reaction temperature in Fig. 8. It is evident from the change in the white line of the XANES spectra that the palladium reduction occurred already at around 240 °C. The palladium speciation at the catalyst bed inlet is determined in more detail from XANES spectra by application of LCF and it can be readily seen from Fig. 8(b) that the PdO and Pd0 components change with the increase in temperature. At 225 °C, immediately after calcination at 400 °C for 30 min and at the beginning of the reduction process, it appears that the inlet of the catalyst bed was almost completely oxidised as evident from the low presence of a metallic Pd phase fraction (2.1%). This was determined by LCF and indicates that the calcination was effective. During the temperature-resolved reduction, the isosbestic point (i.e., the point at which the phase composition of two species is equal) is observed at 246 °C. These results reveal that the reduction of palladium oxide at the inlet of the catalyst bed was gradual.
These observations are further corroborated by the FT of the EXAFS (Fig. 8(c)). At 225 °C the catalyst at the bed inlet presents two peaks at ca. 1.5 Å (phase shift uncorrected) in the first and at ca. 3 Å in the second coordination shells, respectively, attributable to Pd–O and Pd–Pd bonds of PdO like species. The presence of these two peaks at 225 °C suggests that the catalyst was mainly in the oxidised state, consistent with XANES. During the temperature-resolved reduction of the catalyst, the characteristic peak of the Pd–Pd in the first coordination shell of metallic Pd emerges at around 2.4 Å (phase shift uncorrected), with the concomitant progressive decrease of the PdO peaks in the first coordination shell at around 1.5 Å (phase shift uncorrected), which indicates the reduction of palladium oxide to metallic Pd. The amplitude of the metallic Pd–Pd peak in the first coordination shell establishes at around 250 °C, which is in excellent agreement with XANES and LCF.
The outlet region of the catalyst bed was investigated in a similar way after re-calcination of the catalyst, and results are reported in Fig. 9. It is evident from the change in the white line of the XANES spectra (Fig. 9(a)) that the palladium reduction occurred at around 280 °C, which is at higher temperature compared to the bed inlet (Fig. 8). This could be ascribed to the re-calcination before the second temperature-resolved reduction, which might have sintered the catalyst. The metal palladium speciation at the outlet can be seen in Fig. 9(b). At the beginning of the second reduction, it appears that the catalyst bed was not completely oxidised as evident from the presence of a metallic Pd phase fraction (9.9%). This suggests that the first calcination was more effective than the second one.
The isosbestic point is observed at 285 °C, unlike for the inlet bed location (246 °C). However, it is important to note that the occurrence of metallic Pd above 300 °C was the same (ca. 92%) at the inlet and outlet of the catalyst bed, for the first and second calcination respectively. The FT of the EXAFS (Fig. 9(c)) shows the characteristic peak of the Pd–Pd in the first coordination shell of (2.4 Å) emerging at around 290 °C and at 300 °C the Pd phase dominated at the outlet bed position. These results indicate that spatial information along the catalyst bed could be derived employing this novel microreactor, enabling the user to avoid averaging out the information along the catalyst bed, which is typically the case with conventional spectroscopic cells used for XAS measurements.
The gas phase features significantly dominate the spectra collected using the commercial Harrick DRIFTS cell (Fig. 10(c)) and the gas phase fingerprints of methane and carbon dioxide bands appear at 3016 cm−1 and 2300–2360 cm−1, respectively. As also shown in previous IR studies of methane combustion, methane and carbon dioxide are predominantly detected in their gaseous forms.67–69 The absence of strong gas phase bands in the infrared spectra collected with the microreactor is attributed to the lack of dead volume in the microreactor, unlike in the commercial DRIFTS cell. The lack of a gas-filled head space (i.e. dead volume) above the catalyst bed effectively minimises the interference of gas phase bands from the bands arising from the surface adsorbed species, making the microreactor ideal for transient response operando DRIFTS studies.36
Bowker elucidated the CO “light-off”, using X-ray photoelectron spectroscopy over Pd catalyst during CO oxidation.73 At low temperature the surface coverage is dominated by adsorbed CO, which poisons the catalyst and prevents oxidation. However, at a certain temperature molecular oxygen starts adsorbing and dissociating into atoms, which react with adsorbed CO to produce CO2. This process frees four free sites for further oxygen adsorption, making the reaction self-accelerating. Therefore, the abrupt disappearance of the CO band can be ascribed to the complete conversion of adsorbed CO, which at high temperature could not be detected by DRIFTS due to its fast reaction with oxygen. Based on these results, CO adsorbed on the catalyst surface hinders the activation of oxygen below 180 °C and above this temperature oxygen activation starts to take place, with CO oxidation light-off observed in the MS results.
Fig. 12 shows reactor outlet concentrations and DRIFTS spectra collected between 50 and 300 °C during CO oxidation over the pre-oxidised catalyst. From Fig. 12(a) it is clear that the gas phase CO2 appears at around 200 °C, which coincides with a drop in the CO and O2 concentration in the gas phase, indicating the occurrence of CO oxidation. At around 250 °C, CO disappears from the gas phase, while O2 and CO2 concentrations stabilise. From these results, it is evident that the gas phase conversion profiles of CO, O2 and CO2 shift to ca. 20 °C higher temperatures over the pre-oxidised catalyst as compared to the pre-reduced one reported in Fig. 11. The DRIFTS data show a band at 2086 cm−1 appearing between 50 and 120 °C, which is different from that on the pre-reduced platinum surface (Fig. 11). Above 120 °C, the band at 2086 cm−1 starts to redshift to 2078 cm−1 and a new band appears to emerge at 2060 cm−1. These two bands at 2078 and 2060 cm−1 become prominent at around 135 °C and grow in intensity up to 260 °C during the temperature-resolved oxidation. Above 260 °C the bands disappear abruptly, similar to that observed for the pre-reduced catalyst (Fig. 11), which coincides with the MS results that show complete conversion of CO at around 250 °C.
The logarithmic values of CO consumption rates on the pre-reduced and pre-oxidised catalysts are plotted against the inverse of temperature in Fig. 13. The apparent activation energy is derived from the CO conversion range between 7 and 30%. It is evident from Fig. 13 that the reaction rates and activation energies are of similar magnitudes for both the pre-reduced and pre-oxidised Pt/Al2O3 catalysts. In particular, the activation energy for the pre-reduced catalyst, determined to be ca. 46.6 kJ mol−1, is slightly lower than that observed for the pre-oxidised catalyst (48.4 kJ mol−1). In general, the activation energies are consistent with earlier studies. Different global or apparent activation energies for CO oxidation over Pt catalysts have been reported previously.74–77 An apparent activation energy of 56 kJ mol−1 was reported for the CO oxidation on a pre-reduced 5 wt% Pt/SiO2,77 while a value of 84 kJ mol−1 was reported for calcined 1–2 wt% Pt/Al2O3 catalysts, which was found to be independent of the platinum metal dispersion.74
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0cy01608j |
‡ These authors contributed equally. |
This journal is © The Royal Society of Chemistry 2020 |