Zhao
Wei‡
a,
Jingman
Pang‡
b,
Yuan
Ji
cd,
Xing
Yang
a,
Yundan
Liu
*cd,
Long
Ren
e and
Yun
Zhang
*a
aSchool of Physics and Opto-Electronic Technology, Collaborative Innovation Center of Rare-Earth Optical Functional Materials and Devices Development, Baoji University of Arts and Sciences, Baoji, Shaanxi, 721016, P. R. China. E-mail: zhangyun_xtu@163.com
bDepartment of Chemistry and Chemical Engineering, Baoji University of Arts and Science, Baoji 721016, China
cHunan Key Laboratory of Micro-Nano Energy Materials and Devices, Xiangtan University, Hunan 411105, P. R. China. E-mail: liuyd@xtu.edu.cn
dLaboratory for Quantum Engineering and Micro-Nano Energy Technology and Faculty of Materials and Optoelectronic Physics, Xiangtan University, Hunan 411105, P. R. China
eInstitute for Superconducting and Electronic Materials (ISEM), Australian Institute for Innovative Materials (AIIM), University of Wollongong, Wollongong, NSW 2500, Australia
First published on 16th November 2020
Durable electrolytic hydrogen production at high-current densities (>500 mA cm−2) is required as the basis of industrial scale hydrogen evolution reaction (HER). Electrocatalysts, with the purpose of accelerating HER, however, are far from meeting the requirements of high activity, cost effectiveness, and long-term stability, especially in alkaline media. Herein, a series of ultrafine bi- or tri-metallic Mo-based carbides embedded in a graphitic carbon matrix are synthesized by a direct solid reaction between metal molybdate and dicyandiamide (DCA). The components of the proposed multi-metallic carbides can be controlled in a facile manner by precisely configuring the molybdates with different metal cations, enabling the design of electrocatalysts with optimized active sites for HER. With the carbon layer protecting against corrosion, the as-prepared series of (NixCo1−x)6Mo6C2 carbides presents effective HER performance, in which the optimized stoichiometric sample ((Ni0.2Co0.8)6Mo6C2) requires an overpotential of 100 mV to drive 10 mA cm−2 current density for HER. With this electrocatalyst, a durable current density of 1000 mA cm−2 can be achieved by applying an overpotential of 1.84 V towards HER, which is even lower than the required potential of the Pt/C commercial electrocatalyst (2.12 V) for the same current density.
In recent years, intense efforts have been made in developing effective, long-term durable and earth-abundant metal-based substitutes including carbides,7–12 borides,13 phosphides,14–17 oxides,18–20 nitrides,21–24 chalcogenides25–28 and carbon-based materials.9,29 Among these candidate materials, transition metal carbides (TMCs) have several advantages, such as high electronic conductivity, noble-metal-like electronic structure for catalysis, broad pH applicability and chemical stability.30–37 As a representative among various TMCs, molybdenum carbides (e.g. Mo2C and MoC) have been reported to be some of the most active non-precious metal-based electrocatalysts for HER, due to their similar-band electronic configuration to those of Pt-group catalysts.38,39 Subsequently, it was found that the introduction of other transition metal elements into the transition metal carbides, using the synergistic effect between different transition metals, can optimize the Gibbs free energy and M–H bond energy of hydrogen adsorption40–42 and this type of interfacial structure in the material also accelerates the process of water splitting and active hydrogen bonding, all of which contribute to the enhanced hydrogen evolution catalytic performance.43 Though polymetallic carbides theoretically have many advantages for achieving improvement in intrinsic catalytic activity for electrocatalysis, few carbides with more than two metal ions for alkaline electrocatalytic HER have been reported. Thus, it is highly demanded to develop high-quality polymetallic carbides for practical hydrogen production.
In this work, we developed a general route to “synthesize” a series of ultrafine Mo-based HER-active bi-/tri-metallic “carbides” as electrocatalysts by “direct” carbonization of multi-metal “molybdate” precursors. The unique framework crystal structure of molybdates in the form of AMoO4 offers the capability to construct multi-metal compounds, and the multi-metal components can be adjusted to achieve regulation of the electronic configuration and thereby the catalytic activity. Following this strategy, various bimetallic and trimetallic Mo-based carbides, Fe3Mo3C, Co6Mo6C2, Mo6Ni6C, and (NixCo1−x)6Mo6C2, were synthesized. As typical developed examples for HER, a series of ultrafine (NixCo1−x)6Mo6C2 nanocrystals with a small size of 4 nm was grown by using dicyandiamide (DCA) as a carbon source, resulting in a nano-architectural carbide uniformly embedded in a conductive carbonaceous matrix with high chemical and mechanical stability. With the carbon layer protecting against corrosion and accelerating interfacial charge transfer, the as-prepared series of (NixCo1−x)6Mo6C2 carbides presents effective HER performance, in which the optimized stoichiometric sample (Ni0.2Co0.8)6Mo6C2 requires an overpotential of 100 mV to drive 10 mA cm−2 current density for alkaline HER. Using such an electrocatalyst, a durable current density of 1000 mA cm−2 can be achieved by applying an overpotential of 1.84 V towards HER, which is even lower than the potential required by the Pt/C commercial electrocatalyst (2.12 V) for the same current density, demonstrating its good potential for industrial HER application.
(NixCo1−x)6Mo6C2 samples were synthesized by high-temperature carbonization. In a typical procedure, 0.5 g of dicyandiamide (DCA) was firstly dissolved in 5 mL of H2O at 100 °C under magnetic stirring to form a transparent solution. Then, 50 mg of NixCo1−xMoO4 was added to the above hot solution, which was then stirred and boiled until all water evaporated. A dry powder was obtained. Afterwards, the powder was placed in an alumina boat, heated in a pipe furnace at 500 °C for 30 min under a N2 atmosphere with a heating rate of 2 °C min−1, and then further heated at 900 °C for 6 h with a heating rate of 5 °C min−1.
The addition of DCA is regarded to not only act as the carbon source in the final high-temperature carbonization step for crystallization of the carbides, but also as the partitioning and reducing agent for the deoxygenation of the metal molybdate precursors in the first thermal-treatment step, which facilitates the anchoring of intermediate precursors on the carbon-based matrix and the following crystallization without agglomeration.
In view of Ni- and Co-based compounds being active for HER, for the purpose of developing effective electrocatalysts, the following characterization and discussion take the as-prepared (NixCo1−x)6Mo6C2 as examples. The optimized (NixCo1−x)6Mo6C2 catalyst for HER with a particular ratio of Ni and Co could be identified. The microstructure and morphology of (Ni0.2Co0.8)6Mo6C2 as a representative of the (NixCo1−x)6Mo6C2 series were characterized using scanning electron microscopy (SEM) and transmission electron microscopy (TEM).
As shown in the representative SEM images (Fig. 2a and b), (Ni0.2Co0.8)6Mo6C2 nanoparticles are uniformly anchored onto a porous carbon matrix. The relevant X-ray energy-dispersive spectroscopy (EDS) elemental mappings (Fig. 2c–g) illustrate that Co, Mo, Ni, C and N elements as the components of (Ni0.2Co0.8)6Mo6C2 nanoparticles are uniformly distributed. The quantified results also confirmed the ratios of the metal elements, which were consistent with the initial amounts used in the reaction (Fig. S2, ESI†). The TEM image (Fig. 2h) shows that the ultra-small (Ni0.2Co0.8)6Mo6C2 nanoparticles with an average diameter of ca. 4.0 nm are evenly embedded into the N-doped carbon matrix.44,45 The successive lattice fringe with a plane distance of 0.22 nm shown in the high-resolution TEM (HRTEM) image (Fig. 2i) of these particles, which is consistent with the (511) lattice plane of Co6Mo6C2, further confirmed the successful growth of single-phase multi-metal carbides. In addition, these nanoparticles are well enveloped by few-layer graphitic carbon shells (with a typical lattice spacing of 0.36 nm similar to that of graphitic carbon) exhibiting high mechanical and chemical stability. The uniform dispersion of the (Ni0.2Co0.8)6Mo6C2 nanocrystals with an ultra-small size can be ascribed to the confining effect of the N-doped carbon originating from the carbonization of DCA during the reaction and crystallization of the carbides.
Fig. 2 (a and b) SEM images of (Ni0.2Co0.8)6Mo6C2; (c–g) elemental mapping of Co, Mo, Ni, C and N in (Ni0.2Co0.8)6Mo6C2; (h) TEM image of (Ni0.2Co0.8)6Mo6C2; (i) HRTEM image of (Ni0.2Co0.8)6Mo6C2. |
To reveal the chemical state and bonding configuration of the as-prepared (Ni0.2Co0.8)6Mo6C2, X-ray photoelectron spectroscopy (XPS) analysis was carried out, as shown in Fig. 3. The full survey spectrum of (Ni0.2Co0.8)6Mo6C2 confirmed the existence of peaks in the regions of Ni 2p, Co 2p, Mo 3d, O 1s, N 1s, and C 1s (Fig. 3a). For the Co 2p XPS spectra (Fig. 3b), the binding energy peaks of Co 2p3/2 and Co 2p1/2 appear at 781.2 eV and 796.5 eV, respectively. The binding energy peaks at 786.2 eV and 803.4 eV are their corresponding satellite structures (S1 and S2), respectively. In addition, slightly weaker metal Co (Co0) peaks (779.5 eV and 794.7 eV) of (Ni0.2Co0.8)6Mo6C2 could be found, which suggests the formation of cobalt molybdenum bimetallic carbides.46 The spectrum of Mo 3d (Fig. 3c) implies four valence states (0, 2+, 4+, and 6+) for the catalyst. After a curve deconvolution, the doublets of 232.5 eV/232.1 eV and 235.5 eV/234.9 eV can be attributed to 3d3/2/3d5/2 of Mo4+ and 3d3/2/3d5/2 of Mo6+, which stem from the MoO2 and MoO3 species on the (Ni0.2Co0.8)6Mo6C2 nanoframe surface.47 The peak located at 228.8 eV for Mo 3d5/2 can be ascribed to the Mo2+ species, which is assigned to Mo–C bonding.48 The peak located at a binding energy of 227.7 eV is assigned to metallic Mo (Mo0).49 The Mo0 species is derived from the metal (Mo)–metal bond existing in Mo-based carbides, which has already been proved by previous reports.50 For the Ni 2p spectrum (Fig. 3d), the peaks located at 856.1 eV and 871.4 eV with satellite peaks can be assigned to Ni2+ 2p3/2 and Ni2+ 2p1/2 from (Ni0.2Co0.8)6Mo6C2,51 respectively. The details of the C 1s XPS spectra are shown in Fig. 3e. The main peak at 284.2 eV corresponds to the sp2 bonded graphite-like carbon, and the peak at 285.2 eV corresponding to sp3 bonded carbon was also observed. It should be noted that there is only a tiny peak at 288.7 eV, which is ascribed to CO/C–OH groups, indicating that most oxygen containing functional groups of DCA are eliminated during the high temperature treatment and a significant increase in structure ordering of the carbon matrix has been achieved.52 The N 1s spectrum (Fig. 3f) confirmed the N-doping in the carbon matrix including the existence of pyridinic N (397.9 eV) and pyrrolic N (400.2 eV).53
Fig. 3 (a) XPS spectrum of (Ni0.2Co0.8)6Mo6C2, high resolution XPS spectra and the fitted data of Co 2p (b), Mo 3d (c), Ni 2p (d), C 1s (e) and N 1s (f) of (Ni0.2Co0.8)6Mo6C2. |
The electrocatalytic activity of the (NixCo1−x)6Mo6C2 series for HER was systematically evaluated using a standard three-electrode system in 1 M KOH electrolyte. For comparison, the performance of counterparts including DCA-Co, DCA-Mo, Co6Mo6C2 and a commercial 20% Pt/C catalyst was also studied in parallel. The polarization curves in Fig. 4a and Fig. S3 (ESI†) reveal that the Ni/Co/Mo ternary carbides (NixCo1−x)6Mo6C2 possess better electrocatalytic activities towards the HER in comparison to their binary and mono metal carbide counterparts, and (Ni0.2Co0.8)6Mo6C2 exhibits the highest activity among the (NixCo1−x)6Mo6C2 series. To achieve the current density of 10 mA cm−2, as shown in the inset of Fig. 4a, (Ni0.2Co0.8)6Mo6C2 needs an overpotential of 100 mV, which is smaller than those of Co6Mo6C2 (152 mV), DCA-Mo (174 mV) and DCA-Co (245 mV).
In view of practical hydrogen production at an industrial scale, a current density with a higher order of magnitude is usually required for electrolysis operation. Therefore, to probe the potential of the as-prepared ternary carbides for practical applications, the HER activities at a higher current (such as 1000 mA cm−2) of these samples were also evaluated. The overpotential required for the current density of 1000 mA cm−2 using the (Ni0.2Co0.8)6Mo6C2 electrocatalyst is only 1.84 V, which is superior to other carbide counterparts in this work and even better than the performance of the commercial Pt/C (20% Pt) catalyst (2.12 V required for 1000 mA cm−2). It should be noted that although the activity of commercial Pt/C at a low potential (29 mV required for 10 mA cm−2) is better than that of (Ni0.2Co0.8)6Mo6C2, (Ni0.2Co0.8)6Mo6C2 can drive a higher current density when applying a potential over 745 mV. These results suggest that (Ni0.2Co0.8)6Mo6C2 has great potential for practical HER applications.
The Tafel plots were derived from the HER polarization curves by deriving the logarithm of the current density, according to the following equation: η = a + blogj, where η is the overpotential (η10), b is the Tafel slope, and j is the current density. The equation is usually used to evaluate the reaction kinetics in the electrocatalytic hydrogen generation process.54 Hydronium ion reduction consists of three steps: the Volmer, Heyrvosky and Tafel steps, respectively.
Electrochemical hydrogen adsorption (Volmer step)
H2O + M + e− → M–H* + OH− |
M–H* + H2O + e− → M + OH− + H2 |
2M–H* → 2M + H2 |
The Tafel slope is regarded as an intrinsic parameter to reveal the rate determining step in the kinetics of HER. Fig. 4b demonstrates that the Tafel slope of the (Ni0.2Co0.8)6Mo6C2 catalyst is about 59 mV dec−1, while the Tafel slopes of DCA-Co, DCA-Mo and Co6Mo6C2 are 140, 127 and 164 mV dec−1, respectively. Thus, the Volmer–Heyrovsky mechanism is presumed to dominate the HER process when using (Ni0.2Co0.8)6Mo6C2 as the catalyst, and the hydrogen generation rate could be increased rapidly by applying a higher overpotential, resulting in high HER activity with high voltages applied.57,58 To better understand the role of the interface reaction and electrode kinetics for HER, EIS analysis was further employed.59 As the Nyquist plots show in Fig. 4c, the charge transfer resistance Rct of DCA-Co, DCA-Mo, Co6Mo6C2, and (Ni0.2Co0.8)6Mo6C2 is Rct = 25.8 Ω, 18.0 Ω, 11.2 Ω, and 9.42 Ω, respectively. Compared with the other catalysts, (Ni0.2Co0.8)6Mo6C2 displays a much lower Rct, indicating that the addition of Co and especially Ni in the multi-metal carbides significantly enhances the transfer rate of carriers and the faradaic process.60 It is generally believed that the electric double layer capacitance (Cdl) is directly proportional to the electrochemically active surface area (ECSA) during the electrocatalytic process. When there are more effective active components on the catalyst surface, the larger the ECSA, the better the corresponding catalytic activity, so the electric double layer capacitance can often be used to determine the catalyst activity.61 Thus, the CVs of these samples were recorded in the potential range not containing the redox states at different scan rates (10, 20, 30, 50, 70 and 100 mV s−1) in 1 M KOH. As shown in Fig. 4d and Fig. S4 (ESI†), one can clearly observe that the Cdl of (Ni0.2Co0.8)6Mo6C2, Co6Mo6C2, DCA-Mo and DCA-Co is 68.5, 45.4, 12.5 and 6.9 mF cm−2, respectively, manifesting that the Cdl of (Ni0.2Co0.8)6Mo6C2 is the highest, which implies that the multi-metal synergy helps the carbides in exposing more accessible electrochemically active sites.
The catalytic stability is another critical criterion for determining practical HER capability. As shown in Fig. 5a, the stability of the as-prepared (Ni0.2Co0.8)6Mo6C2 was evaluated by a cycling electrochemical test in the form of cyclic voltammetry (CV) sweeps between 0.02 V –and −0.25 V vs. RHE at a scan rate of 50 mV s−1 in 1 M KOH. The negligible change between the polarization curves obtained before and after 2000 continuous CV tests demonstrates the superior stability of (Ni0.2Co0.8)6Mo6C2 in electrochemical processes. The HER durability at a high current density of (Ni0.2Co0.8)6Mo6C2 was also studied by carrying out long-term chronopotentiometry. Only a slight catalytic current depression can be observed after the long-term electrolysis operated at different constant potentials (160 mV, 470 mV, and 650 mV) over 48 hours (Fig. 5b), illustrating the remarkable stability of such ternary carbide catalysts in the alkaline HER process. In comparison, the electrolysis current density driven by the commercial Pt/C catalyst at 650 mV constant potential attenuates by 40% after 15 hours. In addition, considering the demands of practical application, chronopotentiometric curves were recorded for the (Ni0.2Co0.8)6Mo6C2 catalyst by driving a long-term high current density of 1000 mA cm−2. As shown in Fig. 5c, the potential required for maintaining 1000 mA cm−2 remains reasonably stable and lasts over 48 h, suggesting the great potential of the as-prepared (Ni0.2Co0.8)6Mo6C2 for commercial HER utilization. The TEM and XPS characterization results (Fig. S6 and S7, ESI†) of the catalyst after the long-time constant-current HER process demonstrate that the structure and composition of (Ni0.2Co0.8)6Mo6C2 are not obviously changed, showing the good stability of such materials.
Based on the experimental results obtained in this work, it is clear that the synergistic effect between different transition metals in the carbides can optimize the Gibbs free energy and bonding energy of hydrogen adsorption, which then affects the process of water splitting and HER performance. Compared to DCA-Co and DCA-Mo, the Co6Mo6C2 carbides obtained by mixing Co and Mo exhibit improved HER activity. By including Ni in the crystal structure of Co6Mo6C2, the electrocatalytic activity of the multi-metal carbides is further enhanced. The active sites for HER in (Ni0.2Co0.8)6Mo6C2 are significantly increased in relation to the single metal carbides, which can be confirmed by the analysis of the electrochemically active surface areas of different samples. The superior HER activity and durability of (Ni0.2Co0.8)6Mo6C2 in alkaline media can be concluded as due to the synergistic effects of the multi-metal coordinated carbides and the carbon-based architectures. In detail, the following aspects could be outlined: (1) first of all, the small size of (Ni0.2Co0.8)6Mo6C2 ensures a large amount of exposed active sites; (2) double metal cations (Co and Ni) introduce multi-metal synergy to assist fast water dissociation to yield a sufficient amount of protons to accelerate the hydrogen production; (3) the carbon matrix and protective layer derived from DCA offer good chemical and mechanical stability, as well as high interfacial conductivity for the electrocatalysts.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0ma00571a |
‡ These authors contributed equally. |
This journal is © The Royal Society of Chemistry 2021 |