DOI:
10.1039/D6TA00127K
(Paper)
J. Mater. Chem. A, 2026, Advance Article
Atomically dispersed Pt catalyst on ceria-carbon for suppressing C–C cleavage in glycerol electrooxidation
Received
6th January 2026
, Accepted 24th February 2026
First published on 24th February 2026
Abstract
Glycerol, a low-cost and abundant byproduct of biodiesel production, has attracted attention as a feedstock for conversion into value-added chemicals. To maximize the economic value of products, maintaining three carbons (C3) as the dominant product is important yet difficult to achieve at high potentials due to the favorable C–C bond scission. We demonstrate that an atomically dispersed Pt catalyst anchored on defect-rich ceria-carbon selectively controls the glycerol electrooxidation reaction (GEOR), favoring C3 products. The isolated Pt sites favored single-carbon adsorption, preventing multi-carbon binding and subsequent cleavage up until high potential of 1.2 VRHE. The catalyst maintained nearly 70% of C3 selectivity across various potentials with high glycerate productivity and selectivity. In contrast, catalysts with Pt nanoparticles rapidly shifted towards C2 and C1 products, especially glycolate and formate as potential increases. Moreover, Pt single atoms on the catalyst maintained high glycerate productivity without much Pt agglomeration under 48 h operation. Beyond batch operation, the Pt single atom catalyst was validated in a continuous flow-cell reactor. Glycerate remained as the major product, reaching a selectivity of 51.6% as potential increases and exhibited a productivity of 37.0 mmol L−1 mgPt−1 h−1 at 1.2 VRHE. This work highlights atomic dispersion on defect-engineered supports as a powerful strategy to control electrocatalytic pathways in the GEOR via suppressing C–C cleavage.
1. Introduction
In recent decades, the search for alternative energy sources has intensified, driven by the urgent need for clean and sustainable solutions. Alongside renewable power sources such as wind, solar, and tidal energy, attention has also focused on energy carriers, specifically biofuels. For instance, the International Energy Agency (IEA) reported that there would be a near 30% increase in biofuel demand over 2023–2028.1 Among biofuels, biodiesel has become especially prominent due to its abundant sources.2 The most commonly used method for biodiesel production is transesterification and this process inevitably generates about 10 wt% glycerol as a by-product.3 As biodiesel production has expanded rapidly, glycerol has become an abundant co-product, causing persistent oversupply. The glycerol supply is expected to increase faster than its conventional market growth (e.g., food and cosmetics).4,5 In fact, the current estimates suggest that glycerol production is approximately six times greater than the market demand.6 The oversupply of glycerol has significantly reduced its market value, leading the U.S. Department of Energy to designate it as a key biomass-derived platform chemical for the synthesis of oxygenated organic compounds.7,8 As a result, developing efficient strategies to convert glycerol into higher-value chemicals has emerged as a particularly promising approach.
Glycerol electrooxidation (GEOR) using catalysts has emerged as a promising pathway for glycerol valorization.9–11 The conventional heterogeneous catalytic processes require harsh reaction environments involving pressurization and toxic oxidants such as permanganate and nitric acid.12,13 However, the GEOR can be carried out efficiently at room temperature, minimizing the operating cost.14 The primary challenge in the GEOR is the large number of possible reaction pathways, leading to a wide distribution of intermediates and products, including C3 products (glycerate, tartronate, and lactate), C2 products (glycolate, acetate) and C1 products (formate, CO2).15–17 Therefore, the catalyst must be carefully chosen to control product selectivity.
Among various products, achieving high selectivity toward C3 products such as glycerate is important. These molecules preserve the three-carbon backbone of glycerol and possess substantially higher economic value, serving as precursors to fine chemicals, biodegradable polymers, and pharmaceuticals.18,19 Noble metal catalysts, particularly Pt-based materials, exhibit high intrinsic activity toward glycerol electrooxidation.20 Yet, its selectivity depends on various factors, such as catalyst composition,10,12,19 morphology,21,22 and reaction conditions, such as applied potentials23 and temperature.24 To enhance the C3 selectivity even at high potentials, bimetallic Pt alloys are commonly used. Li et al. reported that alloying Pt with Au optimizes the adsorption of the glycerol molecule for one terminal C atom to be adsorbed at the surface, ensuring high C3 selectivity.10 Zhou et al. reported that alloying Pt with Ru facilitates the formation of C3 products while alloying Pt with Rh enhances the formation of C2 products.12 Because the electrooxidation would occur more at high potentials, the C–C bond should be preserved to ensure high C3 productivity even at high potentials.15
In this work, an atomically dispersed Pt catalyst was prepared on defect-rich ceria, which was anchored on a carbon support, to sustain high C3 selectivity. Their activity and selectivity for glycerol electrooxidation were compared with those of Pt nanoparticles deposited on the same defect-rich ceria/C support, Pt clusters immobilized on non-defect-rich ceria/C, and commercial Pt/C catalysts. Pt single atoms provided an ideal active site, which allowed glycerol adsorption for electrooxidation but prohibited C–C bond cleavage. This catalyst with Pt single atoms especially promoted glycerate formation with good C3 selectivity even at a high potential of 1.2 VRHE. Pt nanoparticles promoted C–C bond cleavage, forming more C2 or C1 compounds. The stability of Pt single atoms was tested for 48 h and compared with that of the commercial Pt/C. Notably, the same trend for Pt single atoms was reproduced in a continuous flow-cell configuration, which resembles process-relevant operation more closely and might simplify downstream separation.
2. Experimental
2.1. Materials and chemicals
Chloroplatinic acid hexahydrate (H2PtCl6·6H2O, ≥37.50% Pt basis), ethanol (C2H6O, anhydrous, ≤0.005% water), Nafion perfluorinated resin solution (5 wt% in lower aliphatic alcohols/water), phenol (C6H5OH, ≥99%), and dimethyl sulfoxide ((CH3)2SO, ≥99.5% (GC), DMSO) were purchased from Sigma-Aldrich. Cerium nitrate (Ce(NO3)3·6H2O, 99.99%) was purchased from Kanto chemical. 2-Propanol ((CH3)2CHOH, 99.7%) was purchased from Junsei. Hydrogen peroxide (H2O2, 34.5%) and potassium hydroxide solution (KOH, 1.0 M) were purchased from Samchun Chemical. Toray 090 carbon paper and Vulcan carbon (XC72) were purchased from the Fuel Cell store.
2.2. Catalyst synthesis
The Vulcan carbon was treated with 6 M H2O2 overnight. Then, it was washed, filtered with deionized water, and dried in an oven at 80 °C. Then, 30 wt% ceria was deposited on the treated carbon. An appropriate amount of Ce(NO3)3·6H2O was dissolved in ethanol to prepare a cerium precursor solution. After the treated carbon was dispersed in ethanol, the cerium precursor solution was added and then dried at 85 °C with stirring. The obtained powder was further dried in an oven at 80 °C and heat-treated at 250 °C under N2 flow for 4 h (Ce-C). Ce-C was reduced at 400 °C for 2 h under 10% H2 (N2 balance) to produce CeR-C. Lastly, either 0.3 or 1 wt% of Pt was impregnated on the CeR-C support. The Pt precursor solution was prepared by dissolving an appropriate amount of H2PtCl6·6H2O in ethanol. The support (CeR-C or Ce-C) was dispersed in ethanol, and the Pt precursor solution was subsequently added dropwise under stirring and dried at 85 °C. After reducing the final powder at 250 °C for 1 h under 10% H2 (N2 balance), the catalyst was prepared for evaluation. For comparison, 1 wt% Pt nanoparticles, which were synthesized by a polyol method using ethylene glycol, were deposited on CeR-C (1Pt NP-CeR-C).25
2.3. Characterization
High-angle annular dark field-scanning transmission electron microscopy (HAADF-STEM) was carried out using a Titan cubed G2 60-300 (FEI), operating at an accelerating voltage of 300 kV. X-ray photoelectron spectroscopy (XPS) was performed using K-alpha (ThermoVG Scientific) to analyze the electronic properties of Ce. Binding energies were calculated with respect to C 1s at 284.8 eV. H2-temperature programmed reduction (H2-TPR) was achieved using a BELCAT-B (BELCAT). Ce-C was pretreated with either Ar at 100 °C for 30 min, or with 5% H2 (Ar balance) at 400 °C for 2 h to mimic CeR-C. H2-TPR was performed by increasing the temperature to 900 °C with a rate of 10 °C min−1. X-ray diffraction (XRD) was conducted on a SmartLab (Rigaku) using Cu Kα radiation. The extended X-ray absorption fine structure (EXAFS) was obtained using 8C Nano XAFS and 10C Wide XAFS beamlines at the Pohang Accelerator Laboratory (PAL). The data was processed and simulated using ATHENA and ARTEMIS.
2.4. Electrochemical measurements
All the electrochemical measurements were performed at room temperature using a potentiostat (CHI730E). A Hg/HgO electrode and a carbon rod were used as a reference and a counter electrode, respectively. Before and during the measurements, N2 gas was continuously purged to remove oxygen in the electrolytes. The measured potentials were converted to the reversible hydrogen electrode (RHE) scale and reported in this work using the following equation:
| ERHE = EHg/HgO + 0.059 × pH + 0.098 |
Catalysts were loaded on the carbon paper using a spraying gun and a batch type three-electrode system was used for the electrochemical measurements. A catalyst ink was prepared by sonicating the mixture of catalyst (9 mg), deionized water (0.7 ml), isopropyl alcohol (2.1 ml), and 5 wt% Nafion ionomer solution (128 µl). The catalyst ink was sprayed on carbon paper with a loading of 0.05 mgPt cm−2 and an electrode area of 1 cm2. Before every measurement, 50 cycles of voltage sweep were conducted using a cyclic voltammetry (CV) method in the potential range of 0.05 VRHE to 1.1 VRHE in 1 M KOH with a scan rate of 100 mV s−1. For the methanol oxidation reaction (MOR), an electrolyte of 1 M KOH with 0.5 M methanol was used. It was conducted via the CV method in the same potential range with activation but with a scan rate of 10 mV s−1. The electrolyte was changed to 1 M KOH with 0.1 M glycerol for GEOR measurement. The chronoamperometry (CA) technique was applied at various potentials (0.6, 0.8, 1.0 and 1.2 VRHE) for 3 h to evaluate the catalysts' performance. For the stability test, the CA technique was applied for 48 h at 1.0 VRHE.
To further assess the practical performance of the catalyst, flow cell measurements were conducted. The catalyst ink was sprayed on carbon paper with a loading of 0.05 mgPt cm−2 for the anode and 0.1 mgPt cm−2 for the cathode. The synthesized catalyst and commercial 20% Pt/C were used as the anode and cathode, respectively. A Mini-hydroflex was used as a reference electrode. Either 1 M KOH with 0.1 M or 0.5 M glycerol was circulated at the anode while 1 M KOH was circulated at the cathode, with a flow rate of 10 or 20 sccm. Both electrolytes were purged with N2 gas during the measurement. The CA technique was applied at various potentials for 3 h to evaluate the catalyst performance. The detailed illustrations of the batch system and flow cell are shown in Fig. S1 and S2.
2.5. Product quantification
The GEOR products were collected and examined using an online gas chromatography (GC; Micro GC Fusion, Inficon) system equipped with an Rt-Molecular sieve with a 5 Å column and 1H NMR (Avance Neo 400, Bruker) during and after the CA method, respectively. For gas product quantification, the gas outlet from the GEOR reactor was connected to the GC and GC injections were performed every 5 min. The total productivity of gas products was quantified by integrating a plot of concentration vs. time. For liquid products, the electrolyte after reaction was detected using an NMR spectrometer. A 640 µl sample after the reaction was collected and mixed with 75 µl of D2O. Phenol and DMSO were added as an internal standard. The selectivity of products was estimated using the following equations:
2.6. In situ Raman spectroscopy analysis
In situ Raman spectroscopy was performed using a custom-built electrochemical cell coupled with a Raman spectrometer (InVia™ Qontor confocal Raman microscope, Renishaw). A 532 nm laser was employed with an exposure time of 10 s, 20 accumulations, and a laser power set to 1%. The as-prepared catalysts deposited on carbon paper were used as the working electrode, while a Hg/HgO (1 M KOH) electrode and a Pt wire served as the reference and counter electrodes, respectively, in 1 M KOH electrolyte with 0.5 M glycerol. Raman spectra under steady-state conditions were obtained by multi-step chronoamperometry (CA) from 0.5 to 1.2 VRHE. To observe M–OH peaks, the Raman spectra were captured using a 633 nm laser with an exposure time of 60 s, and 3 accumulations.
3. Results and discussion
3.1. Structural characterization of catalysts
The carbon support was treated with H2O2 to provide surface functional groups. Ceria was then deposited through wetness impregnation followed by thermal treatment, producing a Ce-C support. To enrich surface defects for enabling Pt single atom deposition, this support was further reduced under a H2 atmosphere, yielding a CeR-C support. Subsequently, 0.3 wt% or 1 wt% Pt was loaded on these supports, yielding 0.3Pt-CeR-C or 1Pt-CeR-C, respectively (Fig. 1a). HAADF-STEM showed that no Pt cluster was found in both 0.3Pt-CeR-C and 1Pt-CeR-C catalysts and only Pt single atoms, highlighted with yellow circles, were deposited on ceria (Fig. 1b and c and S3). By contrast, increasing the Pt loading to 1.5 and 2 wt% on CeR-C resulted in predominant Pt clusters (Fig. S4), indicating that 1 wt% is the practical upper limit for stabilizing Pt primarily as single atoms. Pt nanoparticles (2.17 ± 0.24 nm), which were separately synthesized via the polyol method with ethylene glycol, were deposited on the CeR-C support with 1 wt% Pt (1Pt NP-CeR-C) for comparison (Fig. 1d and S5a). When ceria was not reduced, however, both single atoms and clusters (0.86 ± 0.17 nm) were observed in the 1 wt% Pt sample (1Pt-Ce-C; Fig. 1e and S5b). The formation of defect-rich ceria was essential to immobilize Pt single atoms.
 |
| | Fig. 1 (a) Schematic illustration of the synthesis procedure for 1Pt-CeR-C. HAADF-STEM images of (b) 0.3Pt-CeR-C, (c) 1Pt-CeR-C, (d) 1Pt NP-CeR-C, and (e) 1Pt-Ce-C. Yellow, red, and blue circles represent Pt single atoms, Pt clusters, and Pt nanoparticles, respectively. (f) Fourier transform of k3-weighted EXAFS data of various Pt catalysts and the Pt foil reference. | |
Defects in ceria would lead to oxygen vacancies and they provided sites for Pt single atoms to be strongly anchored on.26–28 Compared to Ce-C, CeR-C had a much higher number of defects. XPS results clearly showed that after reduction of ceria, the percentage of Ce3+ increased significantly from 29.2 to 38.8% (Fig. S6). Even after Pt impregnation, the percentage difference was maintained. H2-TPR was additionally conducted to further clarify defect type and abundance (Fig. S7). Two main reduction features were observed at ∼500 °C and ∼715 °C, which are assigned to surface oxygen species and bulk/lattice oxygen, respectively.29 The dominant difference between CeR-C and Ce-C appeared in the surface-related peak, whereas the bulk-related peak showed no change, indicating that the support distinction was mainly associated with surface defects. The integrated H2 consumption in the surface-reduction region was 0.0330 mmol g−1 for CeR-C versus 0.0533 mmol g−1 for Ce-C, suggesting that CeR-C was more pre-reduced at the surface. Both XPS and TPR results support that the higher extent of surface defect sites in CeR-C was the primary contributor to Pt single atom stabilization on ceria-carbon and prevented Pt from being deposited as clusters.
The EXAFS results confirmed that Pt was atomically dispersed on 1Pt-CeR-C and 0.3Pt-CeR-C (Fig. 1f). The presence of the Pt–Cl peak (at 1.9 Å) without the Pt–Pt metallic peak (at 2.6 Å) showed that there were little clusters on those catalysts.30,31 1Pt NP/CeR-C clearly showed a large Pt–Pt peak, similar to that of Pt foil. In the case of 1Pt-Ce-C, the dominant peak was the Pt–Cl bond, but the Pt–Pt bond was still noticeable. From the fitting results of EXAFS data (Table S1), the coordination numbers (CN) for Pt–Pt in 0.3Pt-CeR-C and 1Pt-CeR-C were 0.6 and 0.8, respectively, confirming their single atom feature. However, the CN for Pt–Pt in 1Pt NP-CeR-C was 8.9. Meanwhile, the CN for Pt–Pt in 1Pt-Ce-C was 1.4 which was significantly higher than that of 0.3Pt-CeR-C and 1Pt-CeR-C. These results clearly demonstrate that Pt single atoms were deposited on catalysts with the CeR-C support but both single atoms and clusters co-existed on 1Pt-Ce-C. This is in good agreement with the HAADF-STEM results (Fig. 1b–e). While both 0.3Pt-CeR-C and 1Pt-CeR-C contained Pt single atoms, X-ray absorption near edge spectroscopy (XANES) results showed that Pt on 0.3Pt-CeR-C was more oxidized than that on 1Pt-CeR-C, as evidenced by higher white line intensity (Fig. S8).
3.2. Electrochemical measurements and GEOR
The electrocatalytic performance of the synthesized catalysts and 20% Pt/C was initially investigated in an aqueous solution of 1 M KOH. CVs of the catalysts were recorded in 1 M KOH with a scan rate of 10 mV s−1 and the results are shown in Fig. S9. In 1 M KOH, no distinct hydrogen underpotential deposition (Hupd) peak of Pt was observed for the Pt-ceria-carbon catalysts in the range of 0.05–0.4 VRHE. The Hupd peak was not obvious due to the atomic-sized Pt32 and/or the broad adsorption/desorption peak of ceria in the same range.
The presence of only single atoms on 0.3Pt-CeR-C and 1Pt-CeR-C was further confirmed using the MOR. It is known that the MOR requires at least three consecutive Pt atoms on the surface. Pt ensembles are needed to adsorb methanol and then activate the C–H/C–O bond.33,34 Isolated Pt atoms are not able to provide these contiguous sites and therefore remain inactive toward the MOR. Hence, the MOR can be used as a probe reaction to verify the existence of Pt clusters.35,36 In Fig. S10a, 0.3Pt-CeR-C and 1Pt-CeR-C did not show any activity towards the MOR. However, 1Pt-Ce-C, in which Pt clusters were present, exhibited noticeable MOR activity. 1Pt NP-CeR-C and Pt/C, which contained Pt nanoparticles, showed high MOR activity. The CeR-C support itself did not show any MOR activity, indicating that MOR activity was only from Pt clusters or nanoparticles (Fig. S10b). These MOR results prove that Pt in the 0.3Pt-CeR-C and 1Pt-CeR-C was atomically dispersed without Pt cluster formation.
Next, the GEOR was measured by the CA method. In the aqueous solution of 1 M KOH + 0.1 M glycerol, the catalyst-loaded carbon paper was immersed, and the constant potentials of 0.6, 0.8, 1.0, and 1.2 VRHE were applied for 3 h. The CA curves are presented in Fig. S11. The GEOR on Pt catalysts can produce C3 intermediates of glyceraldehyde (GLD) and dihydroxyacetone (DHA), further oxidized into C3 products of glycerate (GLE), lactate (LA), and tartronate (TAR) (Scheme 1). Under alkaline conditions, DHA rapidly converts to GLD (e.g., via aldol condensation), making it difficult to be obtained in measurable amounts.37,38 These C3 products may be oxidized more into C2 products of glycolate (GLO) and acetate (ACT), or C1 products of formate (FA) and CO2 through C–C bond cleavage.39
 |
| | Scheme 1 GEOR pathways on Pt catalysts. GLD: glyceraldehyde; GLE: glycerate; TAR: tartronate; LA: lactate; GLO: glycolate; ACT: acetate; FA: formate. The products detected in this work are denoted with a red box. | |
Fig. S12 shows the productivities obtained after 3 h of electrooxidation at each potential. The specific productivity and selectivity of each product with detailed glycerol conversion and faradaic efficiency are presented in Table S2. The NMR data and GC results are shown in Fig. S13 and S14. For the catalysts composed predominantly of atomically dispersed Pt, GLE was the most dominant product at every potential. In the case of 1Pt-CeR-C, GLE productivity reached 15.4 mmol L−1 mgPt−1 h−1 at 1.2 VRHE, which was more than twice that at 0.6 VRHE. 0.3Pt-CeR-C and 1Pt-Ce-C also showed a similar trend; the GLE productivity increased as the potential increased. In contrast, for the catalysts with Pt nanoparticles, C2 and C1 products were generated more as the potential increased. 1Pt NP-CeR-C and Pt/C showed GLO, containing two carbons, as their dominant product from 1.0 VRHE. The FA productivity increased significantly upon potential increase for Pt/C, from 1.2 mmol L−1 mgPt−1 h−1 at 0.6 VRHE to 4.9 mmol L−1 mgPt−1 h−1 at 1.0 VRHE. This comparison indicates that Pt single atoms preserved the C3 framework better while Pt nanoparticles cleaved the C–C bond generating more C2 or C1 products.
The C3, C2, and C1 selectivity for various catalysts is summarized in Fig. 2. In most Pt-based catalysts, the high anodic potential facilitates C–C bond cleavage, leading to further oxidized C2 and C1 chemicals.21,39–41 This trend was clearly observed for the catalysts with Pt nanoparticles. The selectivity for C3 products decreased from 60.0% to 39.3% for 1Pt NP-CeR-C, and from 73.9% to 34.9% for Pt/C, respectively (Fig. 2c and e). Similarly, the catalysts with Pt clusters (1Pt-Ce-C, 1.5Pt-CeR-C, and 2Pt-CeR-C) also exhibited a potential-dependent decline in C3 selectivity (Fig. 2d and S15). This further supports that Pt nanoparticles and clusters promote C–C bond scission at elevated potentials.
 |
| | Fig. 2 The selectivity of C3, C2, and C1 at each potential (vs. RHE) for (a) 0.3Pt-CeR-C, (b) 1Pt-CeR-C, (c) 1Pt NP-CeR-C, (d) 1Pt-Ce-C, and (e) Pt/C. The right y-axis (denoted as a green star) reflects the GLE productivity at each potential. (f) The total productivity at each potential. | |
However, it was notable that the selectivity for C3 was nearly maintained in Pt single atoms when the potential increased to 1.2 VRHE, while only slightly decreasing from 83.5% to 77.4% for 0.3Pt-CeR-C, and from 69.7% to 63.6% for 1Pt-CeR-C, respectively. Whereas the C3 selectivity was the highest in 0.3Pt-CeR-C, the GLE productivity was much higher in 1Pt-CeR-C, probably due to more active sites with metallic features. When only GLE selectivity was counted, the difference between Pt single atoms and Pt nanoparticles seemed more pronounced. A decline in GLE selectivity was observed for Pt/C (from 37.1% to 19.1%), whereas an increase in GLE selectivity was observed for 1Pt-CeR-C (from 43.0% to 51.6%) when the potential increased from 0.6 to 1.2 VRHE (Table S2).
When the sum of all the detectable products was considered, the total productivity increased as the potential increased for 1Pt-CeR-C, 0.3Pt-CeR-C, and 1Pt-Ce-C (Fig. 2f). 1Pt-CeR-C especially showed a large increase in the total productivity from 15.3 mmol L−1 mgPt−1 h−1 at 0.6 VRHE to 29.1 mmol L−1 mgPt−1 h−1 at 1.2 VRHE. However, 1Pt NP-CeR-C and Pt/C reached their maximum productivity at 0.8 VRHE and then decreased afterward. In particular, Pt/C presented a significant decrease in the total productivity at 1.2 VRHE, in which the carbon support would be corroded causing Pt detachment.42 The electrochemical surface area (ECSA) truly decreased from 32.4 to 23.1 m2 gPt−1 after the GEOR at 1.2 VRHE for 3 h (Fig. S16a). However, there was no change in CV curves for 1Pt-CeR-C after the same reaction (Fig. S16b). The ceria deposited on the carbon support could act as an electron sink benefiting from the redox cycle between Ce3+ and Ce4+, preventing carbon oxidation.43
The GEOR catalytic properties were further investigated under various electrolyte conditions to evaluate their effect on product selectivity. When the cation effect was evaluated for 1 M KOH, NaOH, and LiOH aqueous solutions (Fig. S17), the GEOR at 1Pt-CeR-C presented little change upon cation change, while Pt/C produced slightly more LA as the cation size decreased. Such cation effects are commonly attributed to differences in the hydration shell that modify interfacial interactions.44,45 Wu et al. proposed that cations selectively associate with glycerol-oxidation intermediates, thereby altering the final product distribution.46 The minimal variation observed for 1Pt-CeR-C suggested that isolated Pt sites were relatively insensitive to the cation effect, compared with Pt nanoparticles. When a neutral electrolyte (pH 7) was used instead of an alkaline electrolyte, the total productivity decreased greatly producing TAR.
3.3. In situ Raman spectroscopy analysis
In order to examine whether the adsorption of glycerol is affected by the Pt atomic configuration, in situ Raman spectroscopy was conducted during the GEOR in 1 M KOH + 0.5 M glycerol at various potentials (Fig. 3a–c and S18). The characteristic C–C stretching vibration modes (νs(C–C)) of glycerol were observed at 819 and 851 cm−1.47 The CH2 rocking vibrations (τ(CH2)) were detected at 913 and 975 cm−1. Bands within 1020–1080 cm−1 and 1088–1130 cm−1 correspond to C–OH stretching (νs(C–OH)) from the terminal and central carbons of glycerol, respectively.48,49 In particular, the sharp peak at 1061 cm−1 was observed when using Pt nanoparticles as a working electrode. Li et al. suggested that the Raman peak at 1061 cm−1 is derived from the glycerol adsorption on the surface via bonding with two terminal C atoms of glycerol molecules, as shown in the left scheme of Fig. 3d.10 The bidentate adsorption of glycerol causes this peak through interaction with 1,3 terminal C atoms and the multiple Pt sites on the Pt nanoparticle. In case of Pt/C, this peak became more distinct with sharpness as the applied potential increased, indicating that glycerol tended to be adsorbed on the Pt surface in a parallel way. In contrast, the catalysts with Pt single atoms showed only a broad peak in the νs(C–OH) stretching band, and there was little change in Raman peaks although potentials were varied. Even with an increase in potential, adsorptions with two terminal carbons were restricted on the Pt single atom catalyst. The single atomic feature probably allowed the adsorption of only one terminal carbon, as shown in the right scheme of Fig. 3d.
 |
| | Fig. 3 In situ Raman spectra recorded for (a) Pt/C, (b) 1Pt-CeR-C and (c) 0.3Pt-CeR-C at varied potentials in 1 M KOH + 0.5 M glycerol. (d) Schematic diagram of glycerol adsorption on a Pt nanoparticle and a Pt single atom. | |
At low potentials, Pt-based catalysts predominantly favor oxidative dehydrogenation, producing GLE as the main product.21,50 At elevated potentials, C–C bond cleavage becomes more favorable, and conventional Pt catalysts typically produce C2 or C1 chemicals, mainly GLO and FA.51 Anil et al. demonstrated that the Pt catalyst follows the pathway towards oxalic acid and formic acid at high potentials.52 It was reported that the conversion of GLE (C3 product) to GLO (C2 product) requires the stabilization of multivalent carbon-binding intermediates on the catalyst surface.53 Pt single-atom catalysts do not provide contiguous Pt sites capable of binding multiple carbon atoms of one GLE molecule. Therefore, the Pt single-atom configuration substantially inhibited C–C cleavage, resulting in dominant oxidative dehydrogenation of glycerol to GLE and a diminished GLE → GLO → FA pathway even at high potentials.
Some studies suggested that ceria can promote OH adsorption and facilitate OH spillover to Pt active sites.54,55 To examine whether ceria affected the adsorbates on the catalyst surface, in situ Raman spectra near 460 cm−1 were compared in 1 M KOH with increasing potential (Fig. S19), where both peaks of Pt–OH(ads) and Ce–OH(ads) appear.10,56 Regardless of potentials, 1Pt-CeR-C and Pt/C presented similar spectra, making the role of ceria in the surface reaction inconclusive. Compared with the Pt/C, 1Pt-CeR-C did not show significantly enhanced *OH formation. These results imply that the distinct difference in the GEOR activity would result from a different Pt configuration, not from the existence of ceria.
3.4. Testing catalyst stability and operating in a flow cell
The GEOR was performed at 1.0 VRHE for 48 h to evaluate the catalyst stability of 1Pt-CeR-C and Pt/C (Fig. 4). The initial selectivity, which was observed for the first 3 h, was mostly maintained, reaching GLE productivity of 249 mmol L−1 mgPt−1 at 48 h in 1Pt-CeR-C. The 1Pt-CeR-C catalyst was stable enough to sustain its high C3 selectivity by maintaining Pt single atoms without agglomeration. Fig. S20a shows HAADF-STEM images of 1Pt-CeR-C obtained after 48 h of operation, indicating that the Pt single atoms were still clearly observed. Moreover, ceria maintained its structure without aggregation. The crystalline size of ceria estimated from XRD data via the Scherrer equation remained at 5.8 nm after the reaction (Fig. S21). In the Pt/C, GLO was produced the most in the early stage, but more FA was formed at 48 h. A shift in the products from C3 to C2 to C1 was observed, indicating the eventual cleavage of the C–C bond over time. The Pt nanoparticles were greatly aggregated after reaction for 48 h (Fig. S20b).
 |
| | Fig. 4 The changes in the GEOR products as a function of time for (a) 1Pt-CeR-C and (b) Pt/C at an applied potential of 1.0 VRHE for 48 h in 1 M KOH + 0.1 M glycerol. | |
Beyond batch operation, flow cell configurations are regarded as an industrially relevant operation because they couple high-rate chemistry with continuous processing.57 The flow cells can enhance mass activity and faradaic efficiency by reducing diffusion-layer thickness and mitigating ohmic losses.58 Moreover, continuous flow enables immediate downstream separation and integration with inline separation technologies.59 Hence, to better approximate industrial operation, the GEOR of 1Pt-CeR-C at various potentials was tested further using a flow cell, whose scheme and photograph are shown in Fig. 5a. Even using the flow cell, 1Pt-CeR-C maintained its high C3 selectivity and high GLE selectivity (50.6%) even at the potential of 1.2 VRHE (Fig. 5b). Moreover, the flow cell assisted to achieve higher GLE productivities than the batch reactor, due to minimized charge transfer resistance. The distance between the anode and cathode was significantly reduced to ∼5 mm in the flow cell. The GLE productivity reached up to 21.7 mmol L−1 mgPt−1 h−1 at 1.2 VRHE. The i–t curves recorded using the flow cell are shown in Fig. S22. The specific productivity and selectivity of each product with detailed glycerol conversion and faradaic efficiency are presented in Table S3.
 |
| | Fig. 5 (a) A scheme and a photograph of the flow cell. (b) The selectivity and GLE productivity for the GEOR of 1Pt-CeR-C for 3 h using the 1 cm2 flow cell in 1 M KOH + 0.1 M glycerol. (c) I–t curve with cumulative GLE productivity of 1Pt-CeR-C for a 100 h stability test using the 5 cm2 flow cell at 1.0 VRHE in 1 M KOH + 0.5 M glycerol. Electrolytes were refreshed every 24 h. | |
Additionally, to evaluate and optimize the key flow-cell parameters, control experiments were conducted by varying the electrolyte flow rate and glycerol concentration (Fig. S23 and Table S4). The potential of 1.2 VRHE was applied for 3 h to maximize the productivity. Increasing the flow rate from 10 sccm to 20 sccm led to a negligible change in productivity. In contrast, increasing the glycerol concentration from 0.1 M to 0.5 M resulted in a significant increase in GLE productivity, reaching 37.0 mmol L−1 mgPt−1 h−1, with a GLE selectivity of 51.6% at 1.2 VRHE. The GLE productivity was compared with the literature values in Table S5, showing that our value of maximum GLE productivity is even higher than the best values reported so far.
To address the feasibility of industrial application, long-term stability was evaluated using an enlarged 5 cm2 flow cell. A chronoamperometric test was conducted at 1.0 VRHE for 100 h (Fig. 5c). 1Pt-CeR-C maintained stable current throughout 100 h of operation, indicating sustained electrochemical activity under prolonged applied potential. Importantly, the catalyst exhibited continuous product formation throughout the 100 h operation, suggesting that catalyst degradation and poisoning barely occurred during the stability test. High cumulative GLE productivity was achieved with 3290 mmol L−1 mgPt−1 at 100 h. The high C3 selectivity was also maintained, indicating that C–C cleavage was suppressed during the extended operation (Table S6).
4. Conclusions
This work demonstrates that the structural nature of Pt – whether atomically dispersed or in nanoparticles – dictates the selectivity of glycerol electrooxidation in alkaline media. Pt single atoms were stabilized on defect-rich ceria, which was immobilized on carbon supports. This catalyst exhibited high C3 selectivity, nearly 70% at various potentials, in glycerol electrooxidation and sustained selective GLE formation even at a high potential of 1.2 VRHE. However, Pt nanoparticles on the same support and Pt/C underwent extensive C–C cleavage and C3 product selectivity decreased as potential increased, forming more C2 or C1 products (GLO and FA). In situ Raman spectroscopy results showed that unlike the Pt nanoparticles, the Pt single-atom catalyst did not have a distinct multi-carbon adsorption state, which could suppress C–C bond cleavage. The single atomic feature was stable for long-term GEOR, while Pt nanoparticles in Pt/C were aggregated. The Pt single atom catalyst was further applied in a flow cell, producing outstanding GLE productivity (37.0 mmol L−1 mgPt−1 h−1) with a GLE selectivity of 51.6% at 1.2 VRHE. These findings underline the important role of atomic dispersion of the Pt catalyst in controlling reaction pathways and selectivity for the GEOR.
Author contributions
H. L. proposed, designed and supervised the project. H. R. L synthesized the catalysts, performed characterization, carried out electrochemical analysis, and wrote the manuscript. E. L. and Y. J. H. carried out in situ Raman spectroscopy. Y. C. carried out STEM of the catalysts. J. K., S. J., and S. P. helped with characterization and analysed the data.
Conflicts of interest
There are no conflicts to declare.
Data availability
The data supporting this article have been included as part of the supplementary information (SI). Supplementary information: Fig. S1–S23, Tables S1–S6. See DOI: https://doi.org/10.1039/d6ta00127k.
Acknowledgements
This work was supported by the National Research Foundation of Korea (NRF) funded by the Korean government (MSIT) (RS-2024-00466554 and 2021R1A3B1076715). We appreciate KARA (KAIST Analysis center for Research Advancement) for equipment. The experiments at PLS were supported in part by MSIT and POSTECH.
Notes and references
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Footnote |
| † These authors contributed equally. |
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