Dexin
Chen‡
ab,
Wenlong
Li‡
b,
Junbo
Liu
b and
Licheng
Sun
*bc
aSchool of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, Zhejiang Province, China
bCenter of Artificial Photosynthesis for Solar Fuels and Department of Chemistry, School of Science and Research Center for Industries of the Future, Westlake University, Hangzhou 310030, Zhejiang Province, China
cDivision of Solar Energy Conversion and Catalysis at Westlake University, Zhejiang Baima Lake Laboratory Co., Ltd., Hangzhou 310000, Zhejiang Province, China. E-mail: sunlicheng@westlake.edu.cn
First published on 10th February 2025
Electrooxidation of 5-hydroxymethylfurfural (HMF) to produce the platform molecule 2,5-furandicarboxylic acid (FDCA) provides a promising approach for biomass upgrading and green hydrogen production. However, the slow reaction kinetics and poor stability of the anode catalyst hinder continuous FDCA production in flowing systems at industrial current densities (>200 mA cm−2). Herein, a ligand-modified catalyst, Ni(OH)2–TPA (TPA: terephthalic acid), is synthesized for efficient HMF oxidation, wherein the uncoordinated carboxylate functions as the proton relay center, significantly enhancing oxidation performances. The current density is increased 16-fold compared to that of pure Ni(OH)2, and the faradaic efficiency of FDCA reaches 96.9 ± 0.2% at even 1000 mA cm−2. Consequently, an anion exchange membrane electrolyzer (25 cm2) is constructed that shows a current of 10.3 A at 1.80 V. The system operates stably for over 240 hours at 7500 mA, producing hectogram-level FDCA continuously with an overall productivity of 2.85 kg m−2 h−1. These results offer insightful strategies for designing catalysts and fabricating electrolyzers for industrial applications.
Broader contextProduction of FDCA through HMF electrooxidation is considered a sustainable and promising method to synthesize bio-based plastic polyethylene furanoate (PEF). Previous studies have focused on developing effective electrocatalysts for HMF oxidation in a three-electrode system but they are yet to be investigated under industrial-relevant current density (>200 mA cm−2) and durability (>200 hours) conditions, particularly for continuous FDCA production in flowing systems. Due to the multiple-proton transfer process during HMF oxidation, the reaction kinetics are greatly hampered. Here, we have constructed a ligand-modified catalyst, Ni(OH)2–TPA, for continuous FDCA production in an AEM-based electrolyzer under industrial conditions. Ni(OH)2–TPA significantly promoted HMF oxidation kinetics by accelerating the proton relay process, exhibiting a current density of 850 mA cm−2 in a three-electrode system and a current of 10.3 A in an AEM electrolyzer (25 cm2). The electrolyzer has been proven to run steadily for over 240 hours at 7500 mA, showing continuous FDCA production with a productivity of 2.85 kg m−2 h−1. The excellent activity and stability of this AEM electrolyzer demonstrate its potential for industrial-scale implementation, providing a robust foundation for future catalyst design and electrolyzer development for biomass upgrading. |
Despite this, constructing a HMF oxidation electrolyzer capable of performing at industrial-related current densities still lacks efficient catalysts.6,7 Catalysts based on Ni, Co, and Cu have been broadly investigated for HMF oxidation but failed to meet the demands of a current density of >200 mA cm−2 and a durability of >200 hours, particularly for flowing systems.8 The potential required typically exceeds 1.6 V versus reversible hydrogen electrode (RHE) in a three-electrode configuration and over 2.0 V in an anion exchange membrane (AEM)-based setup.9–11 In an HMFOR electrolyzer with high current densities, the generated proton may create a microenvironment with low local pH at the anode–membrane interface, complicating the evaluation of the electrolyzer's overall performance.12 Hence, developing a robust and high-performance catalyst that features rapid HMF oxidation kinetics is of great importance. Strategies such as element doping, defect engineering, and morphology regulation have been employed to enhance HMF oxidation kinetics, but the improvements are quite limited.13 Achieving superior performance requires operating at a low working potential (<2.0 V), as higher potentials may lead to catalyst overoxidation and dissolution of the metallic center. Achieving a high faradaic efficiency (FE) of FDCA can prevent the generation of bubbles by the competitive oxygen evolution reaction (OER), which prevents the catalyst from detaching from the substrate.14 Therefore, deep insights into the reaction process are necessary to design a practically viable catalyst that meets these requirements.
HMF oxidation involves a multiple-proton transfer process (Scheme 1). Under strong alkaline conditions (pH > 13), the aldehyde group (–CHO) of HMF is initially oxidized to carboxylic acid (–COOH) by transferring one proton in the presence of two OH− ions, making 5-hydroxymethyl carboxylic acid (HMFCA) the first intermediate.15 Subsequently, 5-formyl-2-furancarboxylic acid (FFCA) is formed by dehydrogenating the hydroxymethyl (–CH2OH) group of HMFCA to an aldehyde group involving a two-proton transfer and losing two electrons. Finally, the remaining –CHO is oxidized to –COOH, thereby producing FDCA. Due to the four-proton transfer process, the overall oxidation reactivity would be greatly restricted, requiring excess potentials to drive HMF oxidation with high productivity. In biocatalytic systems, liver alcohol dehydrogenase (LADH) effectively facilitates alcohol dehydrogenation by accelerating proton transfer.16–18 As depicted in Scheme 1a, the proton generated by the hydroxyl group of the substrate (benzyl alcohol) is transferred via oxygen/nitrogen in the residue of Ser-48, cofactor (NAD+), and His-51 through the proton transfer chains (PT1, PT2, and PT3). Here, the oxygen center acts as a proton relay bridge, effectively shuttling the proton and thus enhancing reaction kinetics.
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Scheme 1 (a) 3D structure of LADH (PDB: 1AXG) and the proton transfer process during dehydrogenation. (b) Reaction route of HMF oxidation to FDCA under strong alkaline conditions (left) and bio-inspired proton relay through the TPA ligand of Ni(OH)2–TPA (right). HMFCA: 5-hydroxymethylfurancarboxylic acid; FFCA: 5-formyl-2-furancarboxylic acid. |
Inspired by this, to construct an analogical proton transfer bridge, we have successfully synthesized a ligand-modified Ni(OH)2 catalyst (Ni(OH)2–TPA, TPA: terephthalic acid) for efficient HMF oxidation (Scheme 1b). In situ infrared and Raman spectroscopy analyses have confirmed that the TPA ligand works as the proton relay center, significantly improving the reaction kinetics of HMF oxidation. A current density of 850 mA cm−2 is obtained at 1.55 V vs. RHE, and the FE of FDCA reaches 96.9 ± 0.2% at even 1000 mA cm−2. Ni(OH)2–TPA runs stably for 200 hours in a three-electrode setup and performed well in an AEM-based electrolyzer. The electrolyzer exhibits a current of 10.3 A at 1.80 V and operates steadily for over 240 hours at 7500 mA, enabling continuous FDCA production at the hectogram level. Our findings provide an efficient strategy for designing HMF oxidation catalysts through bio-inspired ligand modification and demonstrate the practicality in industrial-related scenarios.
To further test the applicability of Ni(OH)2–TPA under industrial current densities for HMF oxidation, the FEs were evaluated at elevated current densities and are shown in Fig. 2d. The FEs of all oxidation products (HMFCA, FFCA, and FDCA) remain at 98.9 ± 1.6% at 100 mA cm−2 and 96.9 ± 0.2% at even 1000 mA cm−2 for Ni(OH)2–TPA, which presents high reaction specificity for being applied in practical electrolyzers (Fig. S13, ESI†). However, the FE for Ni(OH)2 is 96.3 ± 1.1% at 100 mA cm−2 and drastically decays to 61.8 ± 2.6% at 1,000 mA cm−2 due to the vigorous OER process. In the presence of 100 mM HMF, the performance of Ni(OH)2–TPA remains consistent throughout six consecutive cycles, where yields and FEs of FDCA are maintained at ∼100% (Fig. 2e and Fig. S14, 15, ESI†). The current density decays from over 500 mA cm−2 to nearly zero with the complete conversion of HMF. The high FEs of FDCA prevent the competition of the OER and eliminate Ni(OH)2–TPA detachment from the substrate by O2 bubbles. In Fig. 2f, the chronopotentiometry (CP) curve obtained at 200 mA cm−2 shows a negligible change for over 200 hours (Fig. S16, ESI†). The nanoflakes are well preserved after the test, indicating the superior stability of Ni(OH)2–TPA as well (Fig. S17, ESI†).
The electrochemical surface area (ECSA) test is carried out through double-layer capacity (Cdl) to analyze the intrinsic activity of the catalysts. Cdl of Ni(OH)2–TPA in KOH solution is measured to be 5.25 ± 0.49 mF cm−2, surpassing 2.62 ± 0.15 mF cm−2 of Ni(OH)2 (Fig. S18, ESI†). After introducing HMF, the Cdl values of both catalysts remain nearly constant, suggesting that the active sites for the OER could also be active for HMF oxidation.26 LSV plots normalized through the ECSA are presented in Fig. 3a, where Ni(OH)2–TPA outperforms Ni(OH)2 as well. Meanwhile, the activity normalized through the area of the Ni3+ reduction peak also confirms its superior intrinsic performance (Fig. S19, ESI†). As shown, Ni sites serve as catalytically active sites for HMF oxidation. Thus, to roughly compare the number of these sites, catalysts are first oxidized at 1.45 V long enough to convert all Ni2+ to Ni3+. The charge passing through the electrode is then recorded by applying a reducing potential at 1.0 V to form Ni(OH)2 from NiOOH. As shown in Fig. 3b, Ni(OH)2–TPA possesses more passed charges (−0.83 C) than Ni(OH)2 (−0.13 C), denoting that the TPA ligand not only merely brings the exposure of active Ni sites as uncovered by the ECSA test, but may also enhance the catalytic efficiency of specific sites for HMF oxidation. This is also validated by the normalization of the current density through the passed charge (Fig. S20, ESI†).
A steady state Tafel slope analysis is further applied to analyze the reaction kinetics during the HMFOR (Fig. 3c). Ni(OH)2 presents a Tafel slope of 84.8 mV dec−1 under a low current window, which increases to 189.7 mV dec−1 at higher current densities, consistent with the LSV results (Fig. 2a). As the external potential is strong enough to generate NiOOH rapidly from Ni(OH)2, the reactivity for HMF oxidation of NiOOH primarily influences the reaction rate, as evidenced by the Ni2+/Ni3+-like oxidation peak in Fig. 2a and 3a.27 In contrast, the Tafel slope of Ni(OH)2–TPA is calculated to be 30.3 ± 13.1 mV dec−1 throughout the given current range, as confirmed by the almost linear increase in LSV plots. This potential-dependent process directly determines the reactivity by the NiOOH generation rate driven by the increased potential.28 This is also reflected by the fast decrease of open-circuit potential (OCP) values, where the oxidized Ni(OH)2–TPA is reduced more rapidly than Ni(OH)2 upon HMF injection at the same given time (Fig. 3d).29
Based on these findings, operando electrochemical impedance spectroscopy (EIS) further elucidates the reaction behavior at the electrode/electrolyte interface during HMF oxidation (Fig. 3e and f).29 In the absence of HMF, the decrease of the phase angle elucidates that Ni(OH)2–TPA exhibits faster interface reaction kinetics during the OER process (Fig. S21 and Note S2, ESI†). After introducing HMF, the signal of Ni2+ oxidation to Ni3+ can be observed in the middle-frequency region (100–102 Hz) at a potential of up to ∼1.35 V, in line with the onset potential for the HMFOR (Fig. 2a). At higher potentials (>1.35 V), signals in the low-frequency region (10−1–100 Hz) refer to the competition of the HMFOR and OER, as reflected by the decreased FEs (Fig. S10, ESI†).30 The overall high phase angle shows hampered HMFOR kinetics at the interface (Fig. S22, ESI†). After introducing TPA, the decreased phase angle indicates enhanced interface reactivity, including electron and proton transfer processes.31 Signals in the middle-frequency region reflect favorable HMFOR, bringing high currents and FEs without OER interference.
Hence, in situ attenuated total reflectance surface-enhanced infrared absorption spectroscopy (ATR-SEIRAS) is applied to monitor the evolution of carboxylate/carboxylic acid under increasing potentials (Fig. 4a). The signal located at 1235 cm−1 is attributed to the C–O–C vibration of the furan ring in HMF, as the enhanced HMF adsorption is the prerequisite for the subsequent oxidation.32 In Fig. 4c, a strong HMF adsorption peak initially emerges at a potential of 1.10 V for Ni(OH)2–TPA, earlier than the weak peak at around 1.20 V for Ni(OH)2. The signal of carboxylate (–COO−) vibration, associated with FDCA (R–COO−K+ salt) adsorption during the HMFOR, appears at 1357 cm−1 over 1.40 V for Ni(OH)2 (Fig. 4b). In contrast, the –COO− signal is present throughout the given potential range for Ni(OH)2–TPA. This can be attributed to –COO− in the TPA ligand and the overlapped FDCA signal generated in the reaction, as confirmed by the ex situ Raman and FT-IR spectra.33 However, when the potential reaches 1.35 V where HMF oxidation initiates, a carboxylic acid (–COOH) signal at 1590 cm−1 is distinctly observed for Ni(OH)2–TPA instead of Ni(OH)2 as the potential grows.34 This excludes the signal of the adsorbed carboxylic group from FDCA, which usually exists as its potassium salt in KOH once it is formed and desorbed. Conversely, the carboxylate is protonated by the released proton from HMF oxidation, which only appears in the presence of TPA.
The same conclusion can also be drawn from the quasi-in situ Raman spectra in Fig. 4d and e. The –COOH peak at 1610 cm−1 is invisible for Ni(OH)2 both with and without HMF from 1.30 to 1.45 V.34 However, this signal is strong for Ni(OH)2–TPA, and its intensity is slightly enhanced at higher potentials. This indicates that the free carboxylate is protonated and accelerates proton transfer during the OER and HMFOR. A pair of Raman bands ascribed to NiIII–O vibration at 479 and 560 cm−1 appears over 1.35 V for both catalysts in KOH, confirming that NiIII–O act as the catalytic active sites. In the presence of HMF, the NiIII–O band is still detectable for Ni(OH)2 (Fig. 4e), while it completely vanishes for Ni(OH)2–TPA throughout the test. NiOOH reacts rapidly with HMF once it is electroformed, showing enhanced oxidation kinetics. The generated protons during fast HMF oxidation are efficiently ferried through TPA to complete the catalytic cycle. To decipher the role of TPA in HMF oxidation, Ni(OH)2 coordinated with benzoic acid (BAC) is synthesized in a similar way, denoted as Ni(OH)2–BAC.35 The XRD results reveal the intercalation of the BAC molecule in the Ni(OH)2 layer (Fig. S23, ESI†). NiIII–O signals can also be observed for Ni(OH)2–BAC in the presence of HMF with elevating potentials, which is similar to that of pure Ni(OH)2, illustrating its sluggish kinetics toward HMF oxidation (Fig. S24, ESI†). Without the uncoordinated carboxylate (Fig. 4f), the HMFOR activity of Ni(OH)2–BAC is far inferior to that of Ni(OH)2–TPA, emphasizing the significance of TPA for proton relay in HMF oxidation. Deuterium kinetic isotope effect (KIE) tests are performed to further reveal the proton transfer behavior in the OER and the HMFOR (Fig. S25, ESI†). Both catalysts show the primary KIE (KIE value >1.5) under these conditions, indicating that proton transfer is likely involved in the rate-determining step (RDS) or directly affects the RDS during catalysis. The lower KIE value of Ni(OH)2–TPA for the OER and HMFOR specifies that Ni(OH)2–TPA is less sensitive to the proton transfer process. Thus, shutting the generated proton by the TPA ligand in this step significantly helps accelerate the overall reaction kinetics (Note S3, ESI†).
To explore the application of Ni(OH)2–TPA under a more industrial-related current density (>200 mA cm−2), an AEM-based HMF oxidation electrolyzer is constructed, featuring Ni(OH)2–TPA as the anode and Ni–Mo/NF as the cathode (Fig. 5a).36 For a 1 cm2 (1 × 1) electrolyzer, a current density of 196 mA cm−2 is achieved for the OER at a cell voltage of 1.80 V in 1.0 M KOH (Fig. S26, ESI†). After introducing 200 mM HMF, current densities of 500 mA cm−2 and 1000 mA cm−2 are achieved at 1.74 and 1.90 V, respectively, which greatly outperform those of Ni(OH)2-based electrolyzers (Fig. S27, ESI†). The preliminary activity of this 1 cm2 device demonstrates its potential for scaled-up HMF oxidation applications. Therefore, an AEM-based electrolyzer with a serpentine flow field featuring 25 cm2 (5 × 5) is assembled accordingly. The configuration of the electrolyzer is provided in Fig. S28 (ESI†) and the performance is shown in Fig. 5b. Large-scale Ni(OH)2–TPA and Ni–Mo/NF (25 cm2) are synthesized on Ni foam with a uniform distribution (Fig. S29, ESI†). The device exhibits a current of 3.0 A in 1.0 M KOH at a cell voltage of 1.80 V, and the current reaches 4.0 A at 1.60 V and 10.3 A at 1.80 V by adding 200 mM HMF. The temperature of the end plate and outlet is around 38 °C and 42 °C, respectively (Fig. 5c), highlighting the significance of thermal management in the future design of larger-scale HMFOR devices.9 This system runs stably for over 240 hours at a current of 7500 mA (300 mA cm−2) (Fig. 5d), making it one of the best devices for HMF oxidation (Fig. S30 and Table S1, ESI†). The initial cell voltage is 1.70 V and remains at 1.68 V after the durability test. Moreover, the morphology and chemical structure of Ni(OH)2–TPA are also well maintained, demonstrating its superior stability throughout the test (Fig. S31–S34, ESI†). Notably, the electrolyte flow rate is moderately lowered to 3.81 ml min−1 to ensure the complete conversion of HMF (Fig. 5d, inset), thus saving on separation costs.37 FDCA exhibits a low FE at a smaller flow rate due to the competing OER process, while the yield of FDCA would decrease by the incomplete conversion of HMF at a higher flow rate (Fig. S35, ESI†). At the optimized flow rate, the FEs of FDCA are higher than 98.32%, while the yields maintain over 98.33% throughout the test (Fig. S36, ESI†). Based on these results, the productivity of FDCA is calculated to be 2.85 kg m−2 h−1, which has provided a lab-based paradigm for scale-up applications. By acidifying the electrolyte collected over a 40-hour test, 277 g of the FDCA powder is obtained with an overall yield of 96.1% (Fig. 5d, inset).
Techno-economic analysis (TEA) further elucidates the merits of electrochemical HMF oxidation modes (Fig. 5d). The HMF cost and renewable energy cost are assumed to be 10k tonne−1 and 0.30 CNY kW h−1, respectively (Section S4, ESI†). The production cost of FDCA depends on the operating current density of the electrolyzer. At 300 mA cm−2 (this work), the FDCA cost is calculated to be 21.0k CNY with 200 mM HMF, which shows great promise for FDCA production. Meanwhile, the FDCA cost slightly elevates at higher electricity costs, which increased from 20.6k CNY at 0.10 CNY kW h−1 to 21.3k CNY at 0.50 CNY kW h−1 (Fig. S37, ESI†). The concentration of HMF also strongly influences the FDCA cost as the overuse of KOH and subsequent acid–base neutralization are major factors (Note S4, ESI†). In comparison, the FDCA costs are 15.5 k CNY and 32.0k CNY with 400 and 100 mM HMF in 1.0 KOH solution, respectively (Fig. S38, ESI†). High HMF concentration effectively lowers the overall cost (Fig. S39, ESI†). As a result, developing electrocatalytic systems featuring higher HMF concentration with lowered HMF cost is necessary for the valorization of FDCA and downstream products, which needs serious consideration in the future. These results provide a promising approach and deep insights into AEM-based HMF electrooxidation in practical devices.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ee05745g |
‡ These authors contributed equally to this work. |
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