Jiang
Ji
ab,
Yinsheng
Wang
ab,
Changsheng
Cao
*b,
Xin-Tao
Wu
b and
Qi-Long
Zhu
*b
aCollege of Chemistry, Fuzhou University, Fuzhou 350002, China
bState Key Laboratory of Structural Chemistry and Fujian Provincial Key Laboratory of Materials and Techniques toward Hydrogen Energy, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Fuzhou 350002, China. E-mail: cscao@fjirsm.ac.cn; qlzhu@fjirsm.ac.cn
First published on 26th April 2023
Replacing the anodic oxygen evolution reaction in water electrolysis with thermodynamically more favorable oxidation reactions is appealing for reducing the energy consumption of hydrogen production but is limited by the lack of efficient yet cost-effective electrodes. Herein, a self-supporting NiFe-based Prussian blue analogue (PBA) electrode (NiFe-PBA-NF) was directly prepared via a facile semi-sacrificial anodic electrodeposition strategy, in which ultrasmall NiFe-PBA nanoparticles were grown uniformly and compactly on the nickel foam (NF) surface. Benefiting from its ingenious structure and the synergistic effect between Ni and Fe sites, the as-prepared NiFe-PBA-NF exhibited excellent electrochemical performance in the urea oxidation reaction (UOR) with a required potential of only 1.375 V to deliver a current density of 100 mA cm−2, outperforming the powdered NiFe-PBA and even the commercial RuO2 catalyst. Moreover, a Ru-NiFe-PBA-NF electrode assembled with ultrathin Ru-doped NiFe-PBA nanosheets was fabricated through further Ru-modification treatment, which exhibited a remarkable electrochemical performance in the hydrogen evolution reaction (HER), even better than that of the commercial Pt/C catalyst. Ultimately, a UOR-coupled energy-saving hybrid water electrolysis system was constructed by employing Ru-NiFe-PBA-NF and NiFe-PBA-NF as the electrodes for the cathodic HER and anodic UOR, respectively, which only requires a cell voltage of 1.36 V to deliver a current density of 10 mA cm−2, far superior to a conventional water electrolysis system. This work provides a novel way to design advanced organic–inorganic hybrid-based electrodes and innovative water electrolysis systems for efficient hydrogen production.
It is well-known that a typical water electrolysis process involves two half-reactions, i.e., the hydrogen evolution reaction (HER) at the cathode and the oxygen evolution reaction (OER) at the anode.10,11 Generally, the sluggish four-electron transfer kinetics and large overpotentials of the OER make it a bottleneck reaction in water electrolysis.12,13 The most straightforward approach to address this issue is to develop efficient OER electrocatalysts.14,15 However, the high thermodynamic potential (i.e., 1.23 V vs. reversible hydrogen electrode (RHE)) of the OER makes it an insurmountable moat to substantially reduce the electric energy consumption of water electrolysis.16 Alternatively, replacing the anodic OER with the thermodynamically favorable urea oxidation reaction (UOR) in a water electrolysis system is expected to significantly reduce the energy input for H2 production while enabling the treatment of urea-rich wastewater, since the thermodynamic potential (0.37 V vs. RHE) of the UOR is much lower compared to the OER.17–21 Nevertheless, the key to improving the performance of a UOR-coupled water electrolysis system remains to be the development of efficient yet cost-effective electrocatalysts for the UOR.
Recently, metal–organic frameworks (MOFs) have been widely used in the field of electrochemistry because of their high surface areas, ordered porous structures, and easily tunable composition and morphology.22–26 However, the Achilles heel of MOFs as electrocatalysts is their poor conductivity and stability. Moreover, most MOFs prepared by conventional methods are in powder form, making organic binders indispensable during the fabrication of working electrodes, which will lead to partial coverage of active sites, and is thus detrimental to the electrocatalytic performance.27,28 Alternatively, direct growth of MOFs on conductive substrates with intimate contact not only facilitates charge transfer but also exposes more accessible active sites, thus leading to enhanced electrochemical performance.29 Although several effective strategies including solvothermal self-assembly have been reported to fabricate MOF-based self-supporting electrodes with significantly promoted electrocatalytic performance,30–32 the complex and tedious synthetic conditions with low controllability in most cases limit their large-scale application.33
Compared with conventional strategies, electrochemical deposition (ECD) techniques including anodic electrodeposition (AED) and cathodic electrodeposition (CED) have been proven to be environmentally friendly and time-saving, and show precise controllability and easy scalability, thus showing great potential in fabricating MOF-based self-supporting electrodes.34–37 More notably, the metal ion sources required for the construction of MOFs can be directly provided from their own metal substrate by the applied electric field due to electrochemical oxidization. Thereafter, the generated metal ions will further react with organic ligands to form MOFs and deposit on the surface of the substrate. For example, by precisely controlling the electrochemical conditions such as the applied potential and reaction time, Liu et al. realized the in situ growth of large-area Cu3(HHTP)2 (HHTP: 2,3,6,7,10,11-hexahydroxytriphenylene) MOF films on Cu (100) foil.38 Moreover, other Cu-MOF films using different ligands can also be synthesized through a similar growth strategy, confirming the effectiveness and universality of this strategy.39 On the other hand, it has been reported that Ni-based catalysts are the most attractive candidates for the UOR under alkaline conditions.40 Therefore, it is appealing to fabricate Ni-MOF-based self-supporting electrodes with excellent UOR performance via ECD techniques. Unfortunately, to the best of our knowledge, there are few reports on the synthesis of Ni-MOFs through electrochemical technologies so far.
Herein, a self-supporting NiFe-MOF-based nanocomposite electrode (NiFe-PBA-NF) composed of ultrasmall NiFe-based Prussian blue analogue (PBA) nanoparticles was prepared for the first time via a semi-sacrificial AED strategy, during which nickel foam (NF) was used as both the Ni source and the substrate, while K3[Fe(CN)6] was used as both the Fe source and the ligand. Notably, the composition and morphology of the NiFe-PBA-NF electrode and its corresponding electrochemical performance can be easily tuned by adjusting the AED conditions (e.g., applied potential and reaction time). When used directly as the working electrode for the UOR, the optimal one displayed excellent performance with a required applied potential of only 1.375 V to deliver a current density of 100 mA cm−2, which is superior to powdered NiFe-PBA and even commercial RuO2. Moreover, the Ru-NiFe-PBA-NF electrode with excellent HER activity was fabricated through further Ru-modification on the NiFe-PBA-NF electrode, in which ultrathin Ru-doped NiFe-PBA nanosheets were uniformly and densely distributed on the NF surface. Consequently, the UOR-coupled water electrolysis system assembled with Ru-NiFe-PBA-NF and NiFe-PBA-NF as the cathode and the anode, respectively, only needs a cell voltage of 1.36 V to deliver a current density of 10 mA cm−2, which is 102 mV lower compared with that for a conventional water electrolysis system.
The electrochemical performances of UOR||HER and OER||HER were evaluated in a two-electrode cell, in which NiFe-PBA-NF and Ru-NiFe-PBA-NF were used as the anode and the cathode, respectively. 1.0 m KOH with or without 0.33 m urea was used as the electrolyte.
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Scheme 1 Schematic illustration of the fabrication of the NiFe-PBA-NF and Ru-NiFe-PBA-NF electrodes. |
Besides its overall composition and morphology, the surface chemical composition and electronic states of NiFe-PBA-NF were further analyzed by X-ray photoelectron spectroscopy (XPS). As shown in the survey spectra (Fig. S16a†), both NiFe-PBA-NF and NiFe-PBA-p are composed of C, N, O, Fe and Ni. In the N 1s spectrum (Fig. 1e), the peak at 398.0 eV is assigned to the CN bond of the CN− species.41 Characteristic Ni 2p peaks in the Ni 2p spectrum (Fig. 1f) appeared at 856.3 eV (Ni 2p3/2) with a satellite peak at 861.5 eV, indicating their 2+ oxidation state. Meanwhile, another peak at 858.6 eV can be attributed to Ni3+ or the Ni–OH bond.29,42 Moreover, the two peaks at around 708.9 and 721.7 eV in the Fe 2p spectrum (Fig. S16b†) demonstrate their +2 oxidation state.43 Notably, the binding energies of the peaks corresponding to the C
N bond, Ni2+ and Fe2+ in NiFe-PBA-NF and NiFe-PBA-p are almost the same, which further confirms the successful growth of NiFe-PBA on the NF surface. Since Ni2+ originates from the electrochemical oxidation of NF, the in situ formed Ni2Fe(CN)6 crystals can tightly adhere to the substrate, which is beneficial to enhance the electrochemical performance.
According to previous studies, the growth of NiFe-PBA on the NF surface should be affected by AED conditions including the applied potential and reaction time.34 As shown in Fig. S4a and b,† at low applied potentials (e.g., 2.0 and 2.5 V), only a few nanoparticles grew randomly on the NF surface due to the low generated Ni2+concentration. Afterward, the Ni2+concentration gradually increased as the applied potential increased, thereby accelerating the nucleation and growth of NiFe-PBA nanoparticles. As a result, dense NiFe-PBA nanoparticles were tightly and uniformly grown on the NF surface (Fig. S4c and d†). However, overgrowth of NiFe-PBA nanoparticles at a too high applied potential (4.0 V) leads to the cracking of the uniform and dense MOF layer (Fig. S4e†), which may be detrimental to the electrocatalytic performance. Moreover, it is unsurprising that the reaction time has a similar effect on MOF growth to the applied voltage. As shown in Fig. S5b,† a too short reaction time (1000 s) results in incomplete formation of a dense MOF layer, while a too long reaction time (5000 s) leads to the destruction of the MOF layer (Fig. S5d†). Additionally, the SEM–EDX spectra and SEM–EDX elemental mapping images show that C, O, N, Fe, and Ni are all uniformly distributed throughout the as-prepared NiFe-PBA-NF electrodes with different applied potentials and reaction times (Fig. S2, S3 and S6–S13†). Meanwhile, the Ni/Fe ratio decreases with the increase of applied potential and reaction time (Fig. S14†), further demonstrating the gradual growth of NiFe-PBA nanoparticles, which corresponds to the result mentioned above. Furthermore, the electrochemical performance of the as-prepared NiFe-PBA-NF electrodes was determined in 1.0 m KOH with 0.33 M urea. From the results in Fig. S15,† the NiFe-PBA-NF electrode obtained by electrolysis at 3.0 V for 3000 s displayed the best UOR activity. Therefore, an appropriate applied potential and reaction time are critical for the fabrication of a uniform and robust self-supporting NiFe-PBA-NF electrode with optimal electrochemical performance.
The electrocatalytic OER performance of the as-prepared electrodes was first studied in 1.0 m KOH. As shown in Fig. 2a and S17 and 18a,† a pair of redox peaks corresponding to the Ni2+/Ni3+ couple was clearly observed between 1.0 and 1.5 V. Meanwhile, NiFe-PBA-NF displayed the best OER activity with required overpotentials of only 266 and 338 mV to deliver current density (j) values of 10 and 100 mA cm−2, respectively, outperforming NiFe-PBA@NF (281 and 392 mV) and even the benchmark RuO2@NF catalyst (302 and 427 mV). Further measurements revealed that NiFe-PBA-NF exhibits a lower Tafel slope compared with other electrodes (Fig. S18b†), indicating the improved reaction kinetics, which can greatly improve the OER performance. More notably, when 0.33 m urea was added, accompanied by the disappearance of the oxidation peak, the current densities for all electrodes increased significantly (Fig. 2b and S17†), demonstrating the occurrence of the UOR. Meanwhile, it is worth noting that the onset potentials of the UOR are near those of the oxidation peaks, implying that the UOR should be catalyzed by the in situ generated Ni3+ species, which is consistent with previous studies.18 Therefore, the larger peak area of the oxidation peak in NiFe-PBA-NF would contribute to better UOR activity. As a result, NiFe-PBA-NF exhibited the best UOR activity with required potentials of only 1.339 and 1.375 V to deliver j = 10 and 100 mA cm−2, respectively, which were much lower than those of NiFe-PBA@NF (1.373 and 1.464 V), RuO2@NF (1.369 and 1.623 V), and the most recently reported noble-metal free electrocatalysts (Table S1†), making the as-prepared NiFe-PBA-NF one of the most active MOF-based electrodes for the UOR.
To gain more insight into the enhanced UOR activity, the reaction kinetics were first investigated. As shown in Fig. 2c, the nearly overlapping LSV curves collected at scanning rates from 20 to 120 mV s−1 imply that the UOR is a kinetic controlled process. Therefore, the corresponding Tafel plots were obtained to further analyze the reaction kinetics. As shown in Fig. 2d, NiFe-PBA-NF exhibited a lower Tafel slope (29.66 mV dec−1) compared with NiFe-PBA@NF (39.34 mV dec−1), RuO2@NF (35.81 mV dec−1), and NF (68.40 mV dec−1), suggesting its favorable UOR kinetics. Meanwhile, the charge-transfer kinetics were studied by electrochemical impedance spectroscopy (EIS), and the collected EIS plots are shown in Fig. 2e. Notably, the calculated charge-transfer resistance for NiFe-PBA-NF is much smaller than those of other electrodes, which would accelerate the electrocatalytic process. Furthermore, the measurement of electrochemically active surface areas (ECSAs) reveals that NiFe-PBA-NF possesses more exposed active sites with higher intrinsic activity compared with other electrodes (Fig. S19†). Consequently, the improved charge-transfer and reaction kinetics, as well as the adequate exposure of active sites with high intrinsic activity, synergistically endow NiFe-PBA-NF with excellent UOR performance. Additionally, control experiments show that the concentration of urea has an obvious effect on the UOR activity, where 0.33 M is the optimal value in this work (Fig. S20†).
Besides exhibiting excellent UOR activity, NiFe-PBA-NF also showed pretty good long-term stability. Specifically, it can deliver j = ∼100 mA cm−2 for more than 10 h (Fig. 2f). The gradually decreasing current density should be ascribed to the gradually decreasing urea concentration during continuous electrolysis. At the same time, the morphology and structure of NiFe-PBA-NF after a long-term stability test were further analyzed. As shown in Fig. S21,† the SEM and TEM images show inconspicuous changes after the stability test, implying a robust morphology. However, the drastically changed PXRD patterns and Raman and XPS spectra indicate the complete structural evolution of NiFe-PBA (Fig. S22 and S23). In particular, the signal of Fe 2p XPS sharply decreased, which may be due to the dissociation of ferricyanide ligands from NiFe-PBA during the UOR process. Therefore, we speculate that the in situ generated Fe-doped Ni(OH)2/NiOOH should be the real active species for the UOR, which has been extensively demonstrated previously.26,29
Apart from the OER and UOR in the anode, the electrocatalytic activity for the cathodic HER of NiFe-PBA-NF was also evaluated in alkaline electrolyte. Unfortunately, the HER performance of NiFe-PBA-NF is far behind that of commercial Pt/C (Fig. S24†). As a remedy, the Ru-decorated NiFe-PBA-NF electrode (Ru-NiFe-PBA-NF) was fabricated accordingly, since Ru has a comparable HER activity to Pt in alkaline electrolyte yet is much cheaper.42 Notably, the Ru content in Ru-NiFe-PBA-NF was only 0.79 wt% as determined by inductively coupled plasma atomic emission spectrometry (ICP-AES). The PXRD patterns (Fig. 3a) and Raman spectra (Fig. 3b) indicate that Ru-decorating has no effect on the structure of NiFe-PBA. Meanwhile, the diffraction peaks belonging to Ru-based species are not observed in the PXRD pattern, which may due to the low content and good dispersion of Ru species. Moreover, it is unexpectedly found that ultrathin Ru-decorated NiFe-PBA nanosheets are uniformly anchored on the NF surface, which is quite different from the parent nanoparticulate NiFe-PBA (Fig. 3c and S25†), demonstrating the occurrence of structural reorganization of NiFe-PBA during the Ru-decorating process. The SEM–EDX elemental mapping images show the even distribution of Ni, Ru and Fe throughout the entire Ru-NiFe-PBA-NF (Fig. S26†), illustrating the uniform dispersion of Ru species in Ru-NiFe-PBA-NF. The TEM and HRTEM images (Fig. 3d) show that the lattice spacing of Ru-NiFe-PBA-NF (0.577 nm) is the same as that of NiFe-PBA-NF, implying that the structure of NiFe-PBA remains unchanged after Ru decoration, corresponding to the result of the PXRD pattern. Meanwhile, no obvious metallic or oxidized Ru-based nanoparticles were observed (Fig. 3d and S27†), implying that Ru-based species may exist in Ru-NiFe-PBA-NF in the form of single atoms or ultrasmall clusters. Moreover, from the Ru 3p spectrum of Ru-NiFe-PBA-NF shown in Fig. 3e, the peaks at 462.3 and 484.5 eV are attributed to Ru0, while the peaks at 465.2 and 486.6 eV belong to the Rux+ species, indicating the co-existence of metallic and oxidized Ru species.44 Furthermore, the Ni 2p (Fig. 3f) and Fe 2p (Fig. S28b†) spectra of Ru-NiFe-PBA-NF were also collected. Compared with NiFe-PBA-NF, both Ni 2p and Fe 2p spectra in Ru-NiFe-PBA-NF shifted towards higher binding energy after Ru decoration, demonstrating that partial electrons were transferred from Ni and Fe sites to Ru sites, which will regulate the local electronic structure of the active sites, thereby enhancing the electrochemical performance.
Accordingly, the HER performance of Ru-NiFe-PBA-NF was investigated in 1.0 m KOH with 0.33 m urea. Based on the preliminary experiment, the presence of urea in the electrolyte has little effect on the HER activity of Ru-NiFe-PBA-NF (Fig. S29†). As shown in Fig. 3g, Ru-NiFe-PBA-NF exhibited a boosted HER activity with an ultralow overpotential of 43 mV to deliver j = 10 mA cm−2, which is far superior to NiFe-PBA-NF (286 mV) and NF (306 mV) and comparable to commercial Pt/C (46 mV). More impressively, the needed overpotential to deliver j > 100 mA cm−2 for Ru-NiFe-PBA-NF is even much lower compared with Pt/C, indicating its excellent HER activity. Fig. 3h shows the Tafel plots for the as-prepared electrodes based on their corresponding LSV curves displayed in Fig. 3g. It can be clearly observed that the Tafel slope of Ru-NiFe-PBA-NF is much lower compared with NiFe-PBA-NF and NF within the whole test potential region (Fig. 3h and S30†), indicating the superior HER kinetics for Ru-NiFe-PBA-NF. Notably, the Tafel slope of Ru-NiFe-PBA-NF (85.48 mV dec−1) is slightly higher than that of Pt/C (51.21 mV dec−1) within a low-overpotential region of 0 to 0.05 V. However, within the high-overpotential region larger than 0.18 V (Fig. S30†), the derived Tafel slope for Ru-NiFe-PBA-NF (182.69 mV dec−1) is much lower than that for Pt/C (314.62 mV dec−1), illustrating that Pt/C has more excellent HER kinetics under low j values, while it is inferior to Ru-NiFe-PBA-NF at relatively high j values. Furthermore, as displayed in the EIS plots (Fig. S31a†), the semicircle diameter of Ru-NiFe-PBA-NF is close to that of Pt/C and is much smaller than those of NiFe-PBA-NF and NF, demonstrating the improved charge-transfer kinetics, which is helpful to promote HER performance. Moreover, the measurement of ESCAs shows that Ru-NiFe-PBA-NF is able to expose more accessible active sites with higher intrinsic activity than NiFe-PBA-NF and NF and even Pt/C (Fig. S31b and S32†), which may originate from the synergistic effect of Ru-decorating and the restructured nanosheet morphology. Besides having a notable activity, Ru-NiFe-PBA-NF also showed excellent long-term stability during the HER process. As shown in Fig. 3i, the value of j = ∼10 mA cm−2 can be maintained well without obvious decay during the long-term (>14 h) electrolysis.
Encouraged by the excellent UOR and HER performances of NiFe-PBA-NF and Ru-NiFe-PBA-NF, respectively, an undivided advanced hybrid water electrolysis system (UOR||HER) was constructed by replacing the anodic OER with the UOR, in which NiFe-PBA-NF and Ru-NiFe-PBA-NF were used as the anode and the cathode, respectively. Fig. 4a shows the electrochemical performance of UOR||HER and the conventional water electrolysis system (OER||HER) over the NiFe-PBA-NF||Ru-NiFe-PBA-NF pair. Impressively, it requires only 1.36 V to deliver a current density of 10 mA cm−2 for UOR||HER, which is 0.25 V lower than that for OER||HER (1.61 V), demonstrating the effectiveness of replacing the anodic OER with the UOR to facilitate H2 production in water electrolysis systems. Meanwhile, the UOR ||HER performance of the RuO2@NF || Pt/C@NF pair was measured for comparison. As displayed in Fig. 4b and c, the RuO2@NF||Pt/C@NF pair requires an undesirably higher energy input to output the same current density compared with the NiFe-PBA-NF||Ru-NiFe-PBA-NF pair, especially at high current density. For example, the cell voltages are 1.927 and 2.256 V to deliver current densities of 100 and 200 mA cm−2 for the NiFe-PBA-NF||Ru-NiFe-PBA-NF pair, respectively, which are 564 and 740 mV lower than those for the RuO2@NF||Pt/C@NF pair, respectively. To the best of our knowledge, this performance is superior to most recently reported hybrid water electrolysis systems (including UOR ||HER) by using noble-metal free electrocatalysts as electrodes (Table S2†). Besides having a gratifying activity, the NiFe-PBA-NF||Ru-NiFe-PBA-NF pair also presents fairly good long-term stability toward UOR||HER. As shown in Fig. 4d, it can maintain an output current density of 10 mA cm−2 for 24 h without significant decay, implying its potential application in hybrid water electrolysis devices.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ce00289f |
This journal is © The Royal Society of Chemistry 2023 |