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Research Article  |  Open Access  |  10 Jan 2025

Coke deposition mechanisms of propane dehydrogenation on different sites of Al2O3 supported PtSn catalysts

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Chem. Synth. 2025, 5, 19.
10.20517/cs.2024.43 |  © The Author(s) 2025.
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Abstract

Propane dehydrogenation (PDH) Pt-based catalysts are facing the serious challenge of coke deactivation. The locations would greatly influence the coke formation, while the detailed mechanism is not fully explored. Herein, the coke mechanisms on different locations including Al2O3, Sn, Pt, and Pt-Sn sites were deeply investigated via in situ Fourier transform infrared spectroscopy (FTIR) technology, and the key factors triggering catalyst coke deactivation were proposed. Excessive dehydrogenation of propyl species is a crucial initial step in the formation of coke, whether at metal sites or supports. These propyl species on Al2O3 supports then cyclize to form monocyclic aromatic and bicyclic aromatic species, while those on SnOx sites cyclize to form monocyclic aromatic species. As for the Al2O3 supported PtSn catalysts, the strong dehydrogenation function and the interaction between Pt and Al2O3 supports trigger the complex coke formation mechanism. The surface Pt sites with saturated coordination are prone to coke deposition, leading to rapid deactivation at the initial stage of the reaction. However, the low-coordination Pt sites with ultra-small size are found to be highly resistant to coke formation in the PDH reaction, which selectively catalytic the PDH. Owing to the metal-support interaction, the extensive active hydrogen species generated from Pt can regulate the formation of coke precursors on the Al2O3 supports. Furthermore, the effect of hydrogen co-feed on coke deposition is also explored. The hydrogen co-feed inhibits the coke formation and results in a higher H/C ratio (3.96) for aromatic coke precursors. This study can enhance the understanding of the coke formation in PDH, which is important to designing efficient PDH Pt-based catalysts.

Keywords

Coke mechanism, propane dehydrogenation, Pt-based catalysts, Al2O3, active phase

INTRODUCTION

Pt-based catalysts exhibit excellent catalytic activity in the direct dehydrogenation of propane to propylene, while they face a severe challenge of coke deactivation[1-4]. Frequent regeneration not only involves complex processes and huge energy consumption but also cannot fundamentally resolve the problem of coke deactivation[2,5]. Consequently, researchers have developed extensive optimized strategies from various perspectives to suppress coke deactivation, including constructing active phases, selecting carriers, enhancing interactions between metal and carriers, and controlling reaction pathways[6-10]. Among these, adding tin as a promoter to modify, both electronically and geometrically, the structure of the supported Pt on Al2O3 carriers is an effective approach[6,7]. Although this can alleviate the coke deposition problem to some extent, a large amount of coke still forms on the Al2O3 supported PtSn catalyst. A fundamental resolution to the coke deposition necessitates a deep understanding of the key initiation steps and the dynamic evolution mechanism of coke species in propane dehydrogenation (PDH).

The processes of coke formation are complicated, involving complex surface reactions and various intermediates in the PDH process[11,12]. The specific effect brought by coke accumulation significantly depends on the catalytic system and the location of coke deposition. In Pt-based catalysts, the coke positions have been studied, which are classified into three locations, i.e., metallic Pt, the boundary between the Pt and the support, and the support[13,14]. Researchers have associated different site characteristics with their propensity to cause coke deposition and discovered significant variations in the structure and properties of coke formed at different reaction sites[13].

Coke deposition initiated at metallic Pt active sites mainly originates from their strong dehydrogenation function. According to the current mechanism for the PDH reaction, propane molecules adsorb onto the metal sites and undergo two consecutive dehydrogenations, forming a propylene precursor that strongly adsorbs on the metal sites and undergoes excessive dehydrogenation, leading to the formation of coke[8,15]. Numerous studies indicate that larger Pt particles are prone to coke deposition, compared with the small-sized Pt clusters[16,17]. This is mainly attributed to the strong adsorption of propylene precursors on large-sized Pt particles, resulting in excessive dehydrogenation. Besides, the coordination structure of the Pt active phase can also affect coke formation. The coordination-saturated Pt active sites facilitate side reactions, such as C–C cleavage and deep dehydrogenation, thereby forming coke deposits[6,18].

The carrier is another crucial factor in the initiation of coke deposition[19]. Alumina, used as the carrier in industrial Pt-based PDH catalysts, has pronounced acidic characteristics that enable it to catalyze a series of side reactions, such as oligomerization, cyclization, and condensation of the desorbed product olefins, leading to the formation of coke with a high hydrogen-to-carbon ratio[20]. Numerous studies have shown that reducing the acidity of the carrier can significantly decrease the occurrence of cracking and polymerization reactions, enhance the selectivity for propylene in the modified samples, and markedly inhibit the coke deactivation of catalysts[21]. However, some investigators also proposed that when the acidity of the catalyst is too low, the coke amount increases rather than decreases[13,14]. They attributed it to the synergistic effect between metal and acidic sites that inhibited the formation of coke deposition. Therefore, it is evident that the formation of coke deposition during PDH is influenced by the carrier acidity and the synergistic interaction between the carrier and metal sites.

In addition to metal sites and carriers, the reaction situation is a key factor affecting coke deposition behavior in PDH[8,12,22]. In practical propylene production, hydrogen as a co-feeding gas has been utilized to inhibit the deactivation rate, obviously improving the stability of Pt-based catalysts[23]. This inhibitory mechanism is usually attributed to two main factors: (i) the desorption barrier of propylene can be reduced; (ii) metallic active sites can be preserved with the existence of hydrogen[24]. However, the introduction of hydrogen has a large influence on the properties of metal sites and the support acidity, inevitably leading to different coke deposition behaviors.

Hydrogen dissociates at metal sites and forms metal-hydride species (M-H), which possess different adsorption capabilities for propylene precursors from the metallic active phase, thereby significantly influencing coke deposition[25-27]. The hydrogen spillover caused by the metallic Pt sites, forming active hydrogen species, also significantly impacts coke formation[28,29]. Besides, the spillover of these active hydrogen species onto the carrier can alter its surface properties[30,31], triggering another crucial factor of coke formation. Obviously, different sites and reaction situations substantially influence coke formation in PDH with a high degree of interconnectivity between them. Due to the complex interactions of the various factors and the complexity of the reaction mechanisms, the coke formation mechanisms at different sites in PDH are not yet well understood which evidently limits the progress in research on inhibiting coke deactivation. Revealing the coke formation mechanisms in the Pt-based catalyst system could significantly advance the development of de-coking technologies in the PDH field.

Herein, the Al2O3 supported PtSn catalyst, which is widely used and has excellent performance in PDH, is used as the research object. Starting with the key initiation steps of coke deposition in PDH, the formation mechanisms of coke at different locations are deeply analyzed using a Fourier transform infrared spectroscopy (FTIR) method, and an active site structure that does not undergo coke deactivation is proposed. More specifically, the relations between the location of coke, structures of active phase and coke deactivation mechanism are established. The FTIR spectra can provide very important information on the amount and nature of coke and on its effect on the catalyst acidity.

EXPERIMENTAL

Catalyst preparation

Al2O3 (99%, Sasol Germany GmbH) and Sn-Al2O3 (99%, Sasol Germany GmbH) were calcined at 650 °C for 4 h to make γ-Al2O3 support and Sn-γ-Al2O3, respectively. The obtained catalysts were named as the Al2O3 and Sn-Al2O3. The Sn content of the Sn-Al2O3 sample is 0.3 wt%.

The Pt/Al2O3 catalyst was synthesized by a wet impregnation method, in which the theoretical amount of Pt was 0.5 wt%. First, 13.25 mg of H2PtCl6·6H2O (99.5%, Sinopharm Chemical Reagent Co. Ltd.) were diluted in appropriate amounts of water. Subsequently, the solution containing the metal precursors was impregnated into 1.0 g of the above calcined Al2O3. After impregnation, the samples were stirred for 15 min, maintained at room temperature for 6 h, and then dried at 50 °C for 12 h. This was followed by calcination in 20% O2/N2 at 600 °C for 2 h. Sample reduction was conducted in pure H2 atmosphere at 500 °C for 1 h. The obtained catalysts were named as the Pt/Al2O3. As for the Pt/Sn-Al2O3, the calcined Sn-Al2O3 was chosen as a carrier on which to load the H2PtCl6·6H2O using the same preparation procedure. The obtained catalysts were named as the Pt/Sn-Al2O3.

Catalyst characterization

The crystalline structures of the samples were confirmed using a Bruker D8 Advance X-ray diffraction (XRD) instrument. This analysis was conducted using Cu Kα radiation, characterized by a wavelength of 0.154 nm, under an operating voltage of 3 kV. A transmission electron microscopy (TEM) image was recorded on a JEOL-2100F microscope, which was operated at an accelerating voltage of 200 kV. The analysis utilizing X-ray photoelectron spectroscopy (XPS) was conducted employing an ESCALAB Xi+ instrument from Thermo Fisher Scientific, which utilized Al Kα radiation for the X-ray source. All samples underwent a reduction process at 500 °C for 1 h in an atmosphere of pure H2, after which they were hermetically sealed and stored in vials. The hydrogen temperature programmed reduction (H2-TPR) analysis was executed using a BSD-Chem C200 system. This involved flowing a 10% H2/Ar mixture (with a flow rate of 30 mL/min) over a 100 mg sample (with a particle size of 40-60 mesh), while heating at a rate of 10 °C/min per minute until reaching 700 °C. The hydrogen temperature programmed desorption (H2-TPD) analysis was conducted using a BSD-Chem C200 device. In a typical procedure, 50 mg of the catalyst was initially treated under a 10% H2/Ar flow (30 mL/min) at 500 °C for 2 h, followed by a 30-minute He purge at the same flow rate. To facilitate hydrogen absorption, a H2/Ar mixture was flowed over the catalyst for 30 min at 30 mL/min, followed by a He purge for 1 h. Subsequently, the sample was heated to 700 °C at 5 °C/min under He flows (30 mL/min). The ammonia temperature programmed desorption (NH3-TPD) followed the same experimental procedure. The amount of coke deposited was determined using a STA 449 F3 thermogravimetric (TG) analyzer from NETZSCH. The catalyst, weighing 15 mg, underwent He flow (40 mL/min) at 200 °C for 1 h, followed by a cooldown to room temperature. Subsequently, the catalyst was heated from room temperature to 950 °C at a rate of 5 °C/min under 20% O2/N2 (40 mL/min). Raman spectroscopy was performed to investigate the coke properties on a Thermo Fisher DXR Raman spectrometer with a 532 nm laser beam. The laser power, resolution of the apparatus and data acquisition time were 0.1 mW, 2 cm-1 and 10 s, respectively. An inverted configuration of the Nikon AX was used for the confocal fluorescence microscopy studies. All crystals have been measured using a 100 1.0 AU oil objective lens. The fluorescence images were collected using a Nikon AX scan head connected to laser light sources 405, 488, 561 and 640 nm, while the detection area is full spectrum detection with a photomultiplier tube (PMT).

FTIR spectra were recorded on a Thermo Scientific Nicolet iS50 FTIR spectrometer. All spectra were collected as an average of 64 scans at 4 cm-1 resolutions. The difference spectrum is obtained by subtracting the collected infrared (IR) spectra from the background spectra. (1) CO-adsorption experiment: the sample was initially reduced with H2/Ar (30 mL/min) for 1 h and subsequently cooled to 30 °C. Following this, it was exposed to a 10% CO/Ar mixture until equilibrium was reached. Then, the cell was purged with Ar flow to remove the physically adsorbed CO, with IR spectra being gathered continuously until stabilization; (2) Pyridine-adsorption experiment: the samples were activated at 400 °C for 2 h under a vacuum setup (< 10-3 Pa). The sample was subjected to pyridine vapor at 150 °C for 30 min. FTIR spectra were then recorded after degassing at 150 and 400 °C for 1 h; (3) C3H8-dosing and C3H8/H2-dosing experiment: the sample was reduced at 500 °C for 1 h under 10% H2/Ar (30 mL/min). In Ar atmosphere, the temperature was raised to 600 °C to collect the background spectrum. The pulse experiments were carried out at 600 °C by pulses of pure propane or C3H8/H2 mixture (volume ratio = 1:1) [pulse volume = 0.50 cm3 standard temperature and pressure (STP)] to the in situ cell, which was maintained under Ar flow (30 mL/min). After the pulse, FTIR spectra were continuously recorded for five minutes; (4) The isotope exchange reactions with hydrogen and deuterium (H/D) and C3H8-dosing experiment: the sample was evacuated (< 10-3 Pa) at 400 °C for 1 h, and the background spectrum was collected. Then, the sample was exposed to D2O vapor until adsorption saturation. The completely deuterated sample was fed 500 Pa of propane at 400 °C; (5) C3H8 Multiple pulse experiments: the propane pulse experiment procedure is the same as in Part (3). After pulsing propane at 600 °C, the sample was cooled to 30 °C for CO adsorption, using the procedure in Part (1). Following complete CO desorption, the temperature was raised back to 600 °C for a new round of propane pulsing. The IR spectra after 1-10 rounds of propane pulsing and in-situ FTIR spectra of CO adsorption after rounds 1-2 and 9-10 were recorded.

Catalytic tests

The PDH performance was conducted in a tubular quartz reactor with a fixed bed under atmospheric pressure. The reactor’s temperature was regulated using a Golden Eagle temperature controller (Series 708P). In each test, 0.1 g of the catalyst was utilized. A gaseous mixture containing C3H8 and H2 in a 1:1 volume ratio was introduced over the catalyst layer at 600 °C. Product analysis was performed using an inline gas chromatograph. For the separation and detection of H2, C3H8, C3H6, C2H4, C2H6, CH4, and C4-C6 in the effluent, KB-1 (8 m × 0.32 mm × 0.50 μm) and TDX-01 (3 mm × 1 m) columns were employed. The conversion of propane and the selectivity for the various products were determined by:

Propane conversion:

$$ \mathrm{Conv. \ (\%)=([C_3H_8]_{in}-[C_3H_8]_{out})/[C_3H_8]_{in}\times 100} $$

Selectivity of products:

$$ \mathrm{Selectivity \ (\%)=[C_3H_6]_{out}/([C_3H_8]_{in}-[C_3H_8]_{out})\times 100} $$

where [C3H8]in, [C3H8]out and [C3H6]out were the imported molar concentration of C3H8, the outlet molar concentration of C3H8 and C3H6 in the effluent gas, respectively.

RESULTS AND DISCUSSION

Evolution path of coke precursors on different sites of Al2O3 supported PtSn catalysts

The coke formation on Al2O3 supported PtSn catalysts primarily occurs at metal sites, metal-support interface and supports, with distinct mechanisms at each location. However, the current research on the coke deposition mechanism at different sites and the interactive effects between various sites remain unclear [Supplementary Table 1]. To investigate the coke formation mechanisms at these sites, four model catalysts, Al2O3, Sn/Al2O3, Pt/Al2O3, and Pt/Sn-Al2O3, were designed and prepared. All samples maintain the typical crystal phase structure of γ-Al2O3 [Supplementary Figure 1] but have different active components. These four catalysts exhibit similar crystalline morphology and size [Supplementary Figures 2 and 3].

To investigate the formation mechanism of coke precursors on catalysts, a hyphenated technique combining pulse, high temperature and in situ IR spectroscopy was utilized to analyze the types and formation mechanisms of these precursors [Figure 1]. The pulse experiments were carried out at 600 °C by pulses of pure propane (pulse volume = 0.50 cm3 STP) to the in-situ cell, which was maintained under Ar flow (30 mL/min). After the pulse, FTIR spectra were continuously recorded for five minutes. Table 1 exhibits the summary of the vibrational modes and positions of adsorption peaks. When 0.5 mL of C3H8 is pulsed into the in situ cell at 600 °C, strong absorption peaks at 2,872-2,985 cm-1 attributed to the stretching vibrations of methyl C–H bonds in C3H8 are observed [Figure 1][32,33]. These four catalysts show distinct formation processes of coke precursor due to differences in their active components.

Coke deposition mechanisms of propane dehydrogenation on different sites of Al<sub>2</sub>O<sub>3</sub> supported PtSn catalysts

Figure 1. The coke mechanism of PDH on various locations. FTIR differential spectra following propane pulse adsorption for (A) Al2O3, (B) Sn-Al2O3, (C) Pt/Al2O3 and (D) Pt/Sn-Al2O3. The pulse experiments were carried out at 600 °C by pulses of pure propane (pulse volume = 0.50 cm3 STP) to the in situ cell at Ar (30 mL/min) atmosphere. The yellow dashed line represents the adsorption peak, while the white dashed line represents the inverted peak caused by the occupation of adsorption sites. PDH: Propane dehydrogenation; FTIR: Fourier transform infrared spectroscopy; STP: standard temperature and pressure.

Table 1

Summary of the vibrational modes and positions of adsorption peaks (1,200-4,000 cm-1)

SpeciesVibrational
mode
Band position (cm-1)
This
work
Literature range
Olefinδm (C–H)1,3051,295-1,310[34]
1-Propylidyneδs (C–H)1,372, 1,3871,370-1,377[34,35]
1-Propylidene
2-Propylidene
δs (C–H)1,3961,392-1,398[34,35]
1-Propyl
2-Propyl
δs (C–H)1,4501,450-1,458[34,35]
Benzeneν (C=C)1,4701,450-1,650[43-46]
Naphthaleneν (C=C)1,5451,488-1,545[43-46]
Polyaromaticν (C=C)1,5751,575-1,602[43-46]
Acetone
δs (C–H)
ν (C=O)
δ (C–H)
3,014
1,737
1,440
3,000-3,300[40]
1,668-1,725[40-42]
1,434-1,436[40-42]
Alkyneν (C≡C)2,104-2,1902,100-2,260[43]
Propane
Al2O3
νvs (C=C)2,985-2,8722,875-2,990[44]
νvs (H–O)3,700-3,2003,200-3,700[45]

For the Al2O3 sample, four peaks between 1,372 and 1,450 cm-1 attributed to the bending vibrations of C–H in CH2 and CH3 groups are observed at the initial stage of pulsing propane [Figure 1A]. Specifically, the peak at 1,450 cm-1 is associated with 1-propyl and 2-propyl vibrations, 1,396 cm-1 with 1-propylidene and 2-propylidene, 1,372 and 1,387 cm-1 with 1-propylidyne, and 1,305 cm-1 with olefinic C–H stretching vibration[34,35]. These vibrational peaks persist after Ar purging, indicating chemical rather than physical adsorption. It can be seen that propane undergoes dehydrogenation on the Al2O3 surface. According to NH3-TPD and Py-FTIR results [Supplementary Figures 4 and 5], the Al2O3 possesses numerous medium-strong acid sites[36], predominantly as Lewis acid sites at tri-coordinated Al defect sites [Supplementary Figure 6][37-41]. Therefore, it is believed that propane molecules undergo successive dehydrogenation reactions at these Lewis acid sites of Al2O3. Wang et al. also proposed that this type of tri-coordinated Al defect site with Lewis acidity can catalyze the dehydrogenation of propane[42]. The C–H bonds in propane are activated at AlIII sites, forming an AlIV-C3H7 species. Initially, the C–H bonds in propane are broken by proton abstraction by surface oxygen atoms, leading to bonding of propyl with surface aluminum to form the AlIV-C3H7 surface species. In the second step, β-hydrogen is eliminated from AlIV-C3H7, yielding H2 and propylene products, as illustrated in Scheme 1. Therefore, these 1-propylidene, 2-propylidene and 1-propylidyne formed on Al2O3 are the main precursor triggering coke species. A comparison of the product distribution in PDH for Al2O3 samples reveals that the primary gaseous products are propylene, ethylene, and methane resulting from cracking [Supplementary Figure 7]. With increasing reaction time, the content of ethylene remains higher than that of methane and does not show a significant decline, suggesting that ethylene formed from cracking does not undergo further reactions and is not the key species triggering coke formation. Instead, the formation of coke precursors is due to the deep dehydrogenation of propyl species at strong Lewis acid sites [Scheme 1].

Coke deposition mechanisms of propane dehydrogenation on different sites of Al<sub>2</sub>O<sub>3</sub> supported PtSn catalysts

Scheme 1. Reaction mechanism for PDH on the Al2O3 sample. PDH: Propane dehydrogenation.

Furthermore, the FTIR spectrum of Al2O3 also exhibits absorption peaks at 1,470-1,600 cm-1 and 2,100-2,400 cm-1 [Figure 1A]. The peaks at 1,470 and 1,545 cm-1 are attributed to the C=C stretching vibrations of monocyclic and bicyclic aromatic species, respectively[43-48]. The peaks at 2,190 and 2,300-2,380 cm-1 correspond to the C≡C stretching vibration of alkynes and C=C=C stretching vibrations of dienes. With the increase of reaction time, the peak at 1,470 cm-1 increases first and then shows a declining trend, while the peak at 1,545 cm-1 gradually forms and grows. These results indicate that the coke formation pathway on the Al2O3 surface starts with deep dehydrogenation of propene to form propylidene and 1-propylidyne species, which then gradually cyclizes to form substituted monocyclic aromatic species. As the reaction intensifies, these monocyclic aromatic species further dehydrogenate and cyclize to form polyaromatic species [Scheme 2].

Coke deposition mechanisms of propane dehydrogenation on different sites of Al<sub>2</sub>O<sub>3</sub> supported PtSn catalysts

Scheme 2. Formation mechanism of coke precursors on the Al2O3 sample.

Doping Sn species into alumina alters its acidity. Similar to alumina, Sn-Al2O3 only contains Lewis acid sites, but both its acid amount and strength are significantly higher than those of Al2O3 [Supplementary Figures 4 and 5][49]. XPS results show that the Sn species in Sn-Al2O3 mainly exists in the form of Sn4+ [Supplementary Figure 8]. This is further confirmed by the absence of significant Sn species reduction peaks in H2-TPR of Sn-Al2O3 [Supplementary Figure 9][50]. These results indicate that the main Sn species in Sn-Al2O3 is SnOx. Therefore, the acidity change in the Sn-Al2O3 catalyst primarily originates from SnOx species, which show Lewis acidity. When pulsing propane into the Sn-Al2O3 catalyst, the absorption peaks at 1,396, 1,470, and 1,545 cm-1 intensify [Figure 1B]. The intensities of peaks at 1,470 and 1,545 cm-1 belonging to C=C stretching vibrations for monocyclic and polycyclic aromatic species in Sn-Al2O3 are notably higher than those in Al2O3, indicating that the stronger acid strength and higher acid amount of the Sn-Al2O3 sample lead to the formation of more coke. Notably, the peak strength of monocyclic aromatic does not decrease with the formation of polycyclic aromatics, suggesting that a large amount of monocyclic aromatics forms without further transforming into polycyclic aromatics. Combining the coke formation mechanism on Al2O3 [Scheme 2], polycyclic coke formation primarily originates from coke deposition on the Al2O3 support, while SnOx sites predominantly produce monocyclic aromatic coke precursors. Wang et al. also found that the introduction of SnOx species could facilitate the decarbonylation of acetone to form xylene in Sn-HZSM-5 catalysts[51]. Hence, SnOx sites mainly catalyze the deep dehydrogenation of propane to form monocyclic aromatic coke precursor species [Scheme 3].

Coke deposition mechanisms of propane dehydrogenation on different sites of Al<sub>2</sub>O<sub>3</sub> supported PtSn catalysts

Scheme 3. Formation mechanism of coke precursors on the Sn-Al2O3 sample.

After loading Pt, its strong dehydrogenation capability significantly influences the coke deposition mechanism on the catalyst, warranting a discussion on the formation mechanism of coke precursors on Pt/Al2O3 [Figure 1C]. Compared to Al2O3 and Sn-Al2O3 catalysts [Figure 1A and B], the intensity of δs (C–H) absorption peaks for propylidene and propyl groups at 1,372-1,450 cm-1, and δm (C–H) absorption peaks for olefins at 1,305 cm-1 significantly increase. This indicates intense dehydrogenation reactions of C3H8 molecules at Pt sites with strong dehydrogenation ability, forming a large amount of propyl and olefin species. The intensity of peak at 2,104-2,190 cm-1 increases with the intensification of the peaks at 1,305-1,396 cm-1. Hence, further dehydrogenation of propylidyne can form adsorbed diene or acetylene species, whose further cyclization can produce monocyclic aromatics. Different from the Al2O3 and Sn-Al2O3 catalysts [Figure 1A and B], the Pt/Al2O3 catalyst rapidly forms a strong vibration peak at 1,515 cm-1 at the reaction onset, situated between the peak of polycyclic aromatics at 1,545 cm-1 and the peak of monocyclic aromatics at 1,470 cm-1. This peak is attributed to the cycloalkyl benzene coke precursors[52,53]. As the peak areas of monocyclic aromatics at 1,470 cm-1 and cycloalkyl benzene species at 1,515 cm-1 decrease, the polycyclic aromatic peak at 1,575 increases, suggesting that the polycyclic aromatic coke precursors are primarily derived from the condensation of monocyclic aromatic and cycloalkyl benzene species.

Interestingly, an absorption peak at ~1,737 cm-1 is observed in the Pt/Al2O3 [Figure 1C], which is attributed to the ν (C–O) vibration[54,55]. Concurrently, a significant negative peak appears at 3,600-3,800 cm-1, indicating that the hydroxyl groups in the alumina are occupied. These results suggest that the C in coke precursors is linked to O in Al2O3, forming C–O bonds. Airaksinen et al. and Finocchio et al. also reported the presence of acetone-like species in coke precursors on alumina, which further confirms the formation of the C–O bonds in our study[56,57]. Comparative analysis of the change in these C–O species absorption peaks during the reaction indicates that the concentration of C–O species initially increases rapidly with reaction time, then gradually decreases until it completely vanishes. Notably, the absorption peak of C–O species was only observed in the FTIR difference spectra of Pt/Al2O3 sample, not in Al2O3 or Sn-Al2O3[Figure 1A and B], suggesting a close correlation between the formation of C–O species and Pt active sites in Pt/Al2O3 [Scheme 4A]. Given the strong dehydrogenation capability of Pt active sites, the dynamic changes of C–O species are highly correlated with Pt sites.

Coke deposition mechanisms of propane dehydrogenation on different sites of Al<sub>2</sub>O<sub>3</sub> supported PtSn catalysts

Scheme 4. (A) The deep dehydrogenation of propane at the oxygen species of Al2O3 support in Pt/Al2O3 sample; (B) Formation mechanism of the coke precursor and dehydrogenation mechanism on Pt/Al2O3 in PDH, the red ball and line represent the active hydrogen species; (C) Formation mechanism of the coke precursor and dehydrogenation mechanism on the Pt/Sn-Al2O3 catalyst. PDH: Propane dehydrogenation.

Another significant difference between Pt/Al2O3 [Figure 1C] and Al2O3 [Figure 1A] or Sn-Al2O3 [Figure 1B] is the strong absorption peak at 2,020-2,030 cm-1, which is attributed to Pt–H species or active hydrogen species produced by the activation of hydrogen on Pt sites[58]. The large amount of hydrogen spillover desorption peaks at 200-500 °C in H2-TPD for Pt/Al2O3 further confirms substantial active hydrogen species [Supplementary Figure 10]. There is a correlation between active hydrogen species and C–O species absorption peaks. The formation of active hydrogen species is accompanied by the appearance of C–O species. As the C–O species decrease, the content of active hydrogen species also diminishes, and the corresponding inverted peak at the surface hydroxyl groups becomes significantly smaller. This indicates that active hydrogen spills over from Pt sites to the support surface, reacting with C–O species to form hydrocarbon molecules, thereby restoring the alumina hydroxyl groups [Scheme 4B].

Based on scanning transmission electron microscopy (STEM) [Supplementary Figure 3] and CO adsorption IR spectroscopy [Supplementary Figure 11] results, the geometric effect of Sn leads to a smaller size of metal clusters in the Pt/Sn-Al2O3 catalyst (1.51 nm) compared to Pt/Al2O3 (1.74 nm). XPS and H2-TPR results confirm that Pt species in the Pt/Sn-Al2O3 catalyst exist in a lower coordination number and a partially oxidized state [Supplementary Figures 9 and 12, Supplementary Table 2][59-61]. Correspondingly, the main Sn species in the Pt/Sn-Al2O3 catalyst consist of Sn4+ (495.5, 487.0 eV) accounting for 74.0%, Sn2+ (494.6, 486.2 eV) for 4.4%, and Sn0 (492.7, 484.4 eV) for 21.5% [Supplementary Figure 8, Supplementary Table 3]. In this case, the interface structure between Pt and Sn species primarily comprises the structure of Pt-SnOx-Al2O3, which agrees with the previous results[62-65]. The introduction of Sn effectively regulates the geometric and electronic structures of Pt[66], affecting the formation of coke precursors. As shown in the FTIR spectrum of the Pt/Sn-Al2O3 catalyst [Figure 1D], the vibration peak of olefins at 1,470-1,600 cm-1 is observed, along with absorption peaks for monocyclic and polyaromatic species. There is a dynamic transition from monocyclic to bicyclic naphthalene species. Interestingly, the Pt/Sn-Al2O3 catalyst does not exhibit the absorption peak at 1,575 cm-1, and the overall intensity of its IR absorption peaks is weaker than that of Pt/Al2O3. This suggests that the reactivity of Pt/Sn-Al2O3 is milder, focusing primarily on monocyclic and bicyclic aromatic species rather than the more heavily cyclized polycyclic aromatic hydrocarbons.

The 2,020-2,031 cm-1 region is attributed to the vibrational peaks resulting from the interaction between hydrogen and Pt. Compared to the Pt/Al2O3 catalyst [Figure 1C], the peak of Pt–H species in the Pt/Sn-Al2O3 catalyst is mainly concentrated at a lower wavenumber ~2,020 cm-1, with a lower peak intensity [Figure 1D]. Combined with H2-TPD results [Supplementary Figure 10], the desorption peak area of hydrogen spillover of the Pt/Sn-Al2O3 catalyst is significantly lower than that of the Pt/Al2O3 catalyst. This indicates that the reduction in active hydrogen content due to hydrogen spillover leads to a decrease in peak intensity at the 2,020-2,031 cm-1. In H2-TPD [Supplementary Figure 10], hydrogen spillover occurs at higher temperatures, which are energy-intensive. According to FTIR analysis of vibrational characteristics, the peak at 2,031 cm-1 is assigned to active hydrogen species, while the peak at 2,020 cm-1 is attributed to Pt–H species [Figure 1C and D]. The Pt–H species are an efficient active site for PDH. Correspondingly, there is a slight recovery in the hydroxyl region (3,200-4,000 cm-1) after a reduction in hydroxyl coverage, but this recovery is much less significant than in Pt/Al2O3. This further indicates that SnOx species in the Pt/Sn-Al2O3 catalyst regulate Pt to suppress the formation of active hydrogen. Compared to other catalysts, SnOx species promote the formation of Pt–H bonds, establishing efficient active sites for PDH to propylene [Scheme 4C].

Key factors affecting coke deposition of Al2O3 supported PtSn catalysts

Structures of Pt active phase

The coke formation mechanism on Pt active sites is proposed, but various Pt active sites are observed in in-situ FTIR spectra of CO adsorption which can affect the formation of coke precursors. For instance, the linear adsorption peaks at 2,060 and 2,040 cm-1 correspond to high-coordination and low-coordination Pt species, respectively, and the bridge adsorption peak at 1,800 cm-1 [Supplementary Figure 11]. To investigate the influence of different Pt active phase structures on coke deposition, we designed multiple pulse experiments to observe the correlation between coke precursor generation and the structure of Pt active sites. After pulsing propane at 600 °C, the Pt/Sn-Al2O3 catalyst was cooled to 30 °C for CO adsorption analysis. Following complete CO desorption, the temperature was raised back to 600 °C for a new round of propane pulsing. The IR spectra after 1-10 rounds of propane pulsing [Figure 2] and in-situ FTIR spectra of CO adsorption after rounds 1-2 and 9-10 [Figure 3] were recorded.

Coke deposition mechanisms of propane dehydrogenation on different sites of Al<sub>2</sub>O<sub>3</sub> supported PtSn catalysts

Figure 2. FTIR differential spectra of Pt/Sn-Al2O3 at 600 °C with different numbers of pulses of propane. (A) 4,000-3,200 cm-1; (B) 3,200-2,700 cm-1; (C) 2,700-1,800 cm-1; (D) 1,800-1,200 cm-1. The pulse experiments were carried out at 600 °C by pulses of pure propane (pulse volume = 0.50 cm3 STP) to the in situ cell, which was maintained under Ar flow (30 mL/min) between two successive pulses. The yellow dashed line represents the adsorption peak, while the white dashed line represents the inverted peak caused by the occupation of the adsorption site. FTIR: Fourier transform infrared spectroscopy; STP: standard temperature and pressure.

Coke deposition mechanisms of propane dehydrogenation on different sites of Al<sub>2</sub>O<sub>3</sub> supported PtSn catalysts

Figure 3. FTIR differential spectra of CO adsorption on the Pt/Sn-Al2O3 sample after pulse propane and reaction completion. After each pulse experiment, the sample was cooled to 30 °C, and the spectrum was collected after adsorption and desorption of CO. The temperature was raised to 600 °C for the next propane pulse experiment. The CO adsorption FTIR spectra of periods 1-2 and 9-10 were collected. FTIR: Fourier transform infrared spectroscopy.

Figure 2D shows that with increasing pulse numbers, the intensity of the absorption peaks at 1,470 and 1,545 cm-1 gradually rises, indicating the formation of monocyclic and polyaromatic hydrocarbon species. At the same time, the stretching vibrations of aromatic substituents or unsaturated hydrocarbons at 2,300-2,380 cm-1 (C=C=C) and the stretching vibration of unsaturated hydrocarbons at 2,190 cm-1 (C≡C) slightly increase [Figure 2C], attributed to aromatic substituents and unsaturated hydrocarbon species formed by deep dehydrogenation. This indicates that with the increasing number of pulses, monocyclic and polycyclic aromatic hydrocarbon precursors with alkyl substituents continuously form and deposit on the Pt sites. As the formation of coke precursor species, the gradual decrease in intensity within the 3,767-3,784 cm-1 hydroxyl region suggests that the surface hydroxyl groups of supports are covered by coke precursors [Figure 2A]. Combining the above analysis, a positive correlation is observed between the number of propane pulsing cycles and the content of aromatic species. The reduction in hydroxyl content suggests that coke deposition occurs not only at Pt sites but also on the surface of the Al2O3 support.

The intriguing observation from Figure 2D is that the rate of coke deposition during the first 1-2 pulsing cycles is significantly higher than during the 9-10 cycles. This demonstrates a shift in the coke deposition sites. Therefore, we attempt to elucidate the relationship between coke precursors and various Pt sites using in-situ FTIR spectra of CO adsorption [Figure 3]; the intensity of CO adsorption peaks on Pt active sites decreases as the number of pulsing cycles grows. This suggests that coke precursors poison parts of Pt sites. The linear CO adsorption peak for fresh catalysts is predominantly at 2,060 cm-1, shifting mainly to 2,040 cm-1 after the first pulsing cycle, with the emergence of an adsorption peak at 1,925 cm-1 attributed to CO adsorption on ultra-small Pt clusters[61]. This indicates that surface Pt sites with saturated coordination are firstly poisoned, while smaller-size and low-coordinated Pt sites (edge and corner sites of metal clusters) are not covered by coke deposition. After several pulsing cycles, the CO adsorption peaks are primarily at 2,040 and 1,925 cm-1. It is worth noting that the peak at 2,060 cm-1 completely disappeared, while the peaks at 2,040 and 1,925 cm-1 contain no significant changes after the 9-10th pulsing cycles. In this case, the Pt sites in catalyst mainly consist of small-size and low-coordination Pt active phase, which is unaffected by coke precursors.

This can also be confirmed by the correlation between PDH performance and coke deposition behavior of different Pt clusters [Figure 4]. The initial conversion of propane over the Pt/Al2O3 catalyst is 74.5%, which rapidly decreases to 49.2% after 1 h of reaction, a decline of 25.3% [Figure 4A]. This rapid decrease in activity is due to the extensive coke formed on surface Pt sites with saturated coordination [Figure 3, Supplementary Figure 11]. As coke extensively forms and covers these surface Pt sites with saturated coordination, the decreased rate of propane conversion slows down significantly after 1 h, indicating that the left Pt active sites have a strong capability to inhibit coke formation. These Pt active sites exist as low-coordination Pt sites with ultra-small size [Figure 3, Supplementary Figure 11]. As for the Pt/Sn-Al2O3 catalyst, the Sn can regulate Pt species to form more low-coordination Pt sites with ultra-small size, resulting in a slower deactivation of the Pt/Sn-Al2O3 catalyst. The initial conversion decreases from 33.2% to 22.5%, a reduction of only 10.7% [Figure 4B]. However, due to the electronic regulation of Pt by Sn, the conversion of Pt/Sn-Al2O3 catalyst is also reduced, which is significantly lower than the thermodynamic equilibrium conversion (~52%) under the same reaction condition [Supplementary Figure 7]. To further investigate the stability of the catalyst, a 100 h of PDH reaction was conducted for the Pt/Sn-Al2O3 catalyst [Supplementary Figure 13]. The propane conversion of Pt/Sn-Al2O3 gradually decreases as the reaction progresses, stabilizing at ~8% after approximately 50 h. Integrating these findings, the continued increase in coke deposition precursors and the sustained decrease in hydroxyl content, despite Pt sites no longer being affected, indicate that the carrier surface is the primary site of coke deposition.

Coke deposition mechanisms of propane dehydrogenation on different sites of Al<sub>2</sub>O<sub>3</sub> supported PtSn catalysts

Figure 4. Product distribution of different catalysts as a function of time on stream during PDH for (A) Pt/Al2O3 and (B) Pt/Sn-Al2O3 samples. Dehydrogenation conditions: mcatalyst = 100 mg, C3H8/H2 = 1/1 (2.3 mL/min of propane and 2.3 mL/min of H2), Treduction = 500 °C, Treaction = 600 °C, GHSV = 1,000. PDH: Propane dehydrogenation; GHSV: gas hourly space velocity.

Al2O3 carriers

Figure 5 shows the TG and corresponding differential TG (DTG) curves of catalysts after 3 h of PDH reaction. The degrees of weight loss in various catalysts increase in the order of Al2O3 (1.4%) < Sn-Al2O3 (1.9%) < Pt/Sn-Al2O3 (5.4%) < Pt/Al2O3 (18.5%) [Figure 5A]. The first weight loss peak within the 300-450 °C is attributed to coke at metal sites, while the peak within the 450-600 °C corresponds to coke on Al2O3 supports [Figure 5B]. Despite the lower coke content on the Al2O3, a peak in the high-temperature region suggests the formation of coke on the Al2O3 support. For the Sn-Al2O3 catalyst, weight loss is observed in both high- and low-temperature regions, with the high-temperature peak mainly due to coke on the support surface, and the low-temperature peak associated with monocyclic aromatic coke on SnOx species, as indicated by above FTIR analysis [Figure 1B]. The peaks for the Pt/Al2O3 catalyst are predominantly in the low-temperature region, suggesting that extensive coke deposition occurs on the Pt metal sites. The Pt/Sn-Al2O3 sample shows significant weight loss not only in the 300-400 °C range but also between 500-600 °C, confirming substantial coke accumulation on the Pt/Sn-Al2O3 support. Notably, the coke content on the pure Al2O3 sample is low, whereas the significantly severe coke deposition formed on the Al2O3 support in the Pt/Sn-Al2O3 under the same conditions, and there are distinct differences in the weight loss temperatures. These results further confirm that the introduction of Pt enhances coke deposition on the alumina support due to the synergistic effect of the dehydrogenation function of Pt and the acidity of the alumina support.

Coke deposition mechanisms of propane dehydrogenation on different sites of Al<sub>2</sub>O<sub>3</sub> supported PtSn catalysts

Figure 5. (A) TG profiles under air atmosphere and (B) corresponding DTG profiles of spent Al2O3, Sn-Al2O3, Pt/Al2O3 and Pt/Sn-Al2O3. The inset is the enlarged profiles at 250-600 °C. TG: Thermogravimetric; DTG: differential thermogravimetric.

The Raman spectroscopy was performed to further investigate the coke properties on various sites. Generally, the graphitic degree of coke can be reflected by the ID1/IG ratio (height ratio of D1 and G bands), with a smaller value indicating a higher graphitic degree [Supplementary Figure 14][67]. The ID1/IG ratios for Al2O3, Sn-Al2O3, Pt/Al2O3, Pt/Sn-Al2O3 after 3.3 h of reaction, and Pt/Sn-Al2O3 after 100 h of reaction are 0.96, 0.98, 0.71, 0.89, and 0.72, respectively. The ID1/IG ratios for Al2O3 and Sn-Al2O3 are significantly higher than those for the Pt-based catalysts. In addition, the H/C (mol ratio) values from elemental analysis in Supplementary Table 4 show that Al2O3 (15.85) and Sn-Al2O3 (19.59) have higher H/C ratios than the Pt-based catalysts (< 3.96), indicating higher hydrogen content in coke species. This suggests less graphitic coke on Al2O3 and Sn-Al2O3 than Pt/Al2O3 and Pt/Sn-Al2O3.

Confocal fluorescence microscopy was employed to detect the non-graphitized coke on the catalyst after reactions [Supplementary Figure 15]. The significantly higher fluorescence intensity for Al2O3 and Sn-Al2O3 than Pt-based catalysts indicates their lower graphitic degree, which agrees with the Raman result. As shown in the confocal fluorescence spectrum [Supplementary Figure 15F], the peaks located at 421-481, 486-556, 561-646 and 651-736 nm are attributed to the benzene, naphthalene, anthracene and phenanthrene, benzophenanthrene and triphenylene, and coronene. The types of coke on Al2O3 and Sn-Al2O3 are similar. Interestingly, the Sn-Al2O3 sample has a higher content of benzene species than other samples, indicating that SnOx sites are more prone to forming benzene species, which is consistent with the above FTIR results. The Pt/Al2O3 and Pt/Sn-Al2O3-100h samples did not show polycyclic coke species under fluorescence excitation, indicating that their coke species are mainly graphitized coke. These results suggest that the coke on Al2O3 and Sn-Al2O3 catalysts has a lower graphitic degree, compared with Pt-based catalysts.

To further explore the relationship between the Pt active phase, support acidity, and coke deposition on the support surface, Figure 6 presents the IR difference spectra after extensive isotope exchange reactions with H/D followed by pulsing with 500 Pa of propane for Al2O3 samples. As the reaction time increases, the intensity of the absorption peaks at 1,457-1,608 cm-1 gradually increases, indicating the formation of coke precursor species. Concurrently, the 2,400-2,800 cm-1 region, attributed to O–D stretching vibrations, shows a decreasing trend, while the 3,200-4,000 cm-1 region, corresponding to O–H stretching vibrations, tends to increase. This suggests that the O–D groups on the alumina support participate in the dehydrogenation of reactant molecules, leading to the formation of coke. Consequently, D atoms on the support surface are replaced by H, forming O–H. These data indicate that deep dehydrogenation and cyclization to form aromatic coke precursors occur on the Al2O3 surface, further confirming that the support contributes to the formation of coke precursors. In addition, the deactivation constant for the catalysts shows that the deactivation constant of Al2O3 is slightly higher than that of the catalysts containing Pt [Supplementary Table 5]. This indicates that the active sites on Al2O3 can accumulate coke, leading to catalyst deactivation.

Coke deposition mechanisms of propane dehydrogenation on different sites of Al<sub>2</sub>O<sub>3</sub> supported PtSn catalysts

Figure 6. FTIR differential spectra following propane pulse adsorption for Al2O3 after D2O replacement. The pulse experiments were carried out at 600 °C by pulses of pure propane (pulse volume = 0.50 cm3 STP) to the in situ cell at Ar (30 mL/min) atmosphere. FTIR: Fourier transform infrared spectroscopy; STP: standard temperature and pressure.

The effect of hydrogen co-feed

It is well known that the introduction of H2 can suppress the coke deposits in PDH. Therefore, we pulsed pure propane or C3H8/H2 mixture (volume ratio = 1:1) (pulse volume = 0.50 cm3 STP) to the in situ cell under Ar flow (30 mL/min), and continuously recorded FTIR spectra for 5 min. Figure 7 presents a comparative FTIR difference spectrum of propane and a propane-hydrogen gas mixture, further exploring the impact of H2 on the formation of coke precursor species on the Pt/Sn-Al2O3 catalyst. The absorption peaks attributed to aromatic hydrocarbons ν (C=C) in 1,470-1,600 cm-1 show a significant decrease in intensity [Figure 7B and D], indicating that the introduction of H2 effectively inhibits the formation of aromatic and unsaturated hydrocarbons. Additionally, an observation of the νm (C–H) vibrational peak in the aromatic region of 3,050-3,140 cm-1 further suggests that the aromatic species are dominated by a higher H/C ratio [Figure 7A and C]. The introduction of H2 reduces the content and changes the types of coke precursor species.

Coke deposition mechanisms of propane dehydrogenation on different sites of Al<sub>2</sub>O<sub>3</sub> supported PtSn catalysts

Figure 7. FTIR differential spectra following (A and B) pure C3H8 and (C and D) C3H8/H2 mixture (volume ratio = 1:1) pulse adsorption for Pt/Sn-Al2O3, and corresponding mass spectrum of (E) pure C3H8 and (F) C3H8/H2 mixture pulse. The pulse experiments were carried out at 600 °C by pulses of pure propane and C3H8/H2 mixture (pulse volume = 0.50 cm3 STP) to the in situ cell at Ar (30 mL/min) atmosphere. The yellow dashed line represents the adsorption peak. FTIR: Fourier transform infrared spectroscopy; STP: standard temperature and pressure.

In Supplementary Figure 16, in-situ FTIR spectra of CO adsorption were utilized to investigate the effect of feed composition on Pt sites. The area of the CO adsorption peak at Pt sites in the mixed-feed sample exhibits a lesser decline compared to the propane-only feed, indicating that the presence of H2 inhibits the poisoning of Pt sites by coke deposition. In the mass spectrometry (MS) analysis presented in Figure 7C and D, a significant amount of propylene desorption is detected in the MS when C3H8 is fed alone, coupled with an increase in the intensity of the coke deposition IR peaks, suggesting that deep dehydrogenation on the catalyst leads to coke formation and poisons the Pt sites. Conversely, when the mixed feed is analyzed, a higher content of hydrogenolysis product CH4 is detected, along with a decrease in the intensity of the coke IR peaks, indicating that the coke precursor species on the Pt sites undergo hydrogenolysis, thereby inhibiting the poisoning of Pt sites by coke. The introduction of hydrogen effectively controls and adjusts the content and types of coke precursor species while also preventing the poisoning of Pt sites by coke.

CONCLUSIONS

The formation mechanisms of coke at Al2O3, Sn, Pt and Pt-Sn sites of Al2O3 supported PtSn catalysts in PDH are clarified. Compared to Pt and Pt-Sn sites, the coke initiation capability of Al2O3 and Sn is significantly weaker. The tri-coordinated aluminum with Lewis acidity in Al2O3 is the primary site for coke formation, where propane undergoes excessive dehydrogenation to form propylidene and propylidyne, which further cyclize to form monocyclic and polycyclic aromatic coke precursors. The coke precursors at SnOx sites differ from those on Al2O3, where the propyl species only forms monocyclic aromatic coke precursors after excessive dehydrogenation. For the Pt/Sn-Al2O3 catalyst, the strong dehydrogenation function and the interaction between Pt and supports trigger the complex coke formation mechanism. The coke formation is mainly ascribed to the following three factors: the structures of Pt-Sn clusters, active hydrogen species, Al2O3 support under the influence of active hydrogen species. The surface Pt sites with saturated coordination are prone to coke deposition, while the low-coordination Pt sites with ultra-small size are found to be highly resistant to coke formation in the PDH reaction. The strong dehydrogenation ability of Pt and the active hydrogen species play a vital role in the formation of coke precursors on Al2O3. Hydrogen co-feed also affects the formation of coke precursor. Hydrogen co-feed significantly inhibits the formation of coke precursors and leads to the formation of aromatic hydrocarbon coke precursors with higher H/C ratios. This work can provide the theoretical basis for the development of PDH catalysts with excellent coking resistance performance, and the established research method of coke is expected to be applied to more catalytic research fields.

DECLARATIONS

Authors’ contributions

Designed, prepared and revised the manuscript: Jiao, J., Yang, Y., Song, L.

Discussion and preparation of the manuscript: Jiao, J., Yang, Y., Yuan, M., Tang, X., Shi, M., He, K., Zhang, H., Bi, Y., Qin, Y., Song, L.

Availability of data and materials

The detailed materials and methods in the experiment were listed in the Supplementary Materials. Other raw data that support the findings of this study are available from the corresponding author upon reasonable request.

Financial support and sponsorship

This work was supported by the National Natural Science Foundation of China (No. U1908203; No. U20A20120) and Basic Scientific Research Project of Liaoning Province Department of Education (No. JYTQN2023342).

Conflicts of interest

All authors declared that there are no conflicts of interest.

Ethical approval and consent to participate

Not applicable.

Consent for publication

Not applicable.

Copyright

© The Author(s) 2025.

Supplementary Materials

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Cite This Article

Research Article
Open Access
Coke deposition mechanisms of propane dehydrogenation on different sites of Al2O3 supported PtSn catalysts
Jianhao Jiao, ... Lijuan Song

How to Cite

Jiao, J.; Yang, Y.; Yuan, M.; Tang, X.; Shi, M.; He, K.; Zhang, H.; Bi, Y.; Qin, Y.; Song, L. Coke deposition mechanisms of propane dehydrogenation on different sites of Al2O3 supported PtSn catalysts. Chem. Synth. 2025, 5, 19. http://dx.doi.org/10.20517/cs.2024.43

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