Open Access Article
Renjith
Nadarajan
,
Anju V.
Gopinathan
,
Naduvile Purayil
Dileep
,
Akshaya S.
Sidharthan
and
Manikoth M.
Shaijumon
*
School of Physics, Indian Institute of Science Education and Research Thiruvananthapuram, Maruthamala PO, Thiruvananthapuram, Kerala 695551, India. E-mail: shaiju@iisertvm.ac.in
First published on 6th September 2023
Highly active and earth-abundant electrocatalysts for the hydrogen evolution reaction (HER) and oxygen evolution reaction (OER) are of great significance for sustainable hydrogen generation through alkaline water electrolysis. Here, with an aim to enhance the bifunctional electrocatalytic activity of cobalt molybdate towards overall water splitting, we demonstrate a simple method involving the modulation of the cobalt to molybdenum ratio and creation of phase-modulated heterointerfaces. Samples with varying Co/Mo molar ratios are obtained via a microwave-assisted synthesis method using appropriate starting precursors. The synthesis conditions are modified to create a heterointerface involving multiple phases of cobalt molybdenum suboxides (CoO/CoMoO3/Co2Mo3O8) supported on Ni foam (NF). Detailed electrochemical studies reveal that modulating the composition and hence the interface can tweak the bifunctional electrocatalytic activity of the material for HER and OER and thus improve the overall water splitting efficiency with very high durability over 500 h. To further evaluate the practical applicability of the studied catalyst in water splitting, an alkaline electrolyser is fabricated with the optimized cobalt molybdenum suboxide material (CMO-1.25) as a bifunctional electrocatalyst. A current density of 220 mA cm−2 @1.6 V and 670 mA cm−2 @1.8 V was obtained, and the device showed very good long-term durability.
The platinum group of metals (PGMs) is considered the state-of-art or benchmark catalysts for HER and OER. However, low availability and high cost hamper the widespread use of PGM in commercial applications. In recent years, a variety of catalysts have been explored as efficient and potential replacement for PGM, such as transition metal chalcogenides,9–13 phosphides,14–17 nitrides,18–21 carbides,22–27 borides,28–31 oxides,32–34 catalyst derived from metal–organic frameworks,35–38 covalent organic frameworks39,40 and phthalocyanine.41–45 Most of these materials show good durability and activity in alkaline medium, especially for OER. However, their HER kinetics in alkaline medium is remarkably inferior compared to the acidic medium. Engineering the catalyst surfaces has been shown to be an effective approach towards achieving improved activity towards both HER and OER. Such bifunctional catalyst activity for HER and OER could greatly simplify the system design and lower the cost. Creating heterostructures or hierarchical architectures of components with synergistic effects can modulate the bonding and band structure, improving the catalytic performance.13,46–48 However, building such heterostructures with control on their phase regulation is always challenging and complex.49,50
Transition metal molybdates (TMMoO4) and their hydrates direct lot of interest as electrocatalysts because of the prominent HER activity of Mo-based materials and the flexible electronic structure between Mo and the heteroatoms (TM = Co or Ni or Fe).51–53 MoNi nanoparticle decorated CoMoO3 cuboid arrays on NF as the scaffold (MoNi/CoMoO3/NF) was shown to exhibit high stability and activity, owing to the interaction between different phases as well as the ability to increase the active sites of CoMoO3 cuboids, and the synergistic effect on the whole.53 Bimetallic Ni nanowires and MoNi4/MoO3−x nanorod arrays prepared from NiMoO4 precursor by a thermal reduction method were reported to exhibit comparable HER activity to Pt/C under alkaline conditions.53 Similarly, cobalt molybdenum suboxides (Co2Mo3O8) and their heterostructures supported on nickel as well as cobalt foam have been studied as efficient electrocatalysts for the HER in alkaline electrolytes.52,54–56 Recent study shows that the OER performance of CoO can be further improved by modification with MoO2 due to the synergistic effect between MoO2 and CoO.57 Li et al. reported the 1D MoO2-Co2Mo3O8@C nanorods that showed favourable electrocatalytic advantages toward OER in an alkaline solution.58
The use of a bifunctional catalyst can make the overall system design easier and more cost-effective, and therefore, it is highly necessary to make efficient catalysts for both the HER and OER under alkaline conditions, which still remains a challenge.7 While most of the reports on transition metal molybdate-based electrocatalysts focus on either HER or OER activity, it is to be noted that their bifunctional electrocatalytic activity (towards HER/OER) can be tuned through morphology and phase engineering approaches. Here, with an aim to enhance the bifunctional electrocatalytic activity of cobalt molybdate towards overall water splitting, we demonstrate a simple method involving the modulation of cobalt to molybdenum ratio and creation of phase-modulated heterointerfaces. Samples with varying Co/Mo molar ratios are obtained by using appropriate starting precursors, and the synthesis conditions are modified to create a different heterointerface involving multiple phases of cobalt molybdenum oxide. Detailed comparison studies reveal that modulating the composition and hence the interface can tweak the bifunctional catalytic activity of the material for electrochemical hydrogen evolution and oxygen evolution reaction and thus improve the overall water splitting efficiency.
:
1, 1.25
:
1, 1.5
:
1 and 2
:
1), stirred for 30 min, and the cleaned NF was dipped in this solution and transferred into a 30 mL microwave vial. The sealed glass vial was kept at 180 °C for 45 min and then cooled to ambient temperature. The samples were washed thoroughly with DI water and IPA and then dried at 60 °C. Further, the catalyst samples were annealed at 450 °C under an Ar/H2 flow (100 sccm; 90
:
10) for 2 h. According to the weight change of the sample after annealing, the average loading of the catalyst on NF was determined to be nearly 0.8 mg cm−2.
Potential cycling is typically done with a sweep rate of 50 mV s−1 before measuring the polarization curves. The polarization curves were measured by linear sweep voltammetry (LSV) at a scan rate of 2 mV s−1 to evaluate the HER and OER performance of working electrodes. Electrochemical impedance spectroscopy (EIS) measurements were carried out in a frequency range of 100 kHz to 10 mHz with an amplitude of 5 mV. The Cdl value was measured using the cyclic voltammetry (CV) method, based on which the electrochemical active surface area (ECSA) of the catalysts was determined.
:
1, 1.25
:
1, 1.5
:
1, and 2
:
1, and the formed samples are referred as CMO-1, CMO-1.25, CMO-1.5 and CMO-2, respectively. Optimized samples were grown on NF with varying geometrical area for the electrochemical measurements (Fig. 1b). Systematic studies revealed that the phase composition of the samples synthesized via microwave-assisted route was independent of the molar ratio of Co/Mo precursors at least in a range of 1
:
1 to 2
:
1 (Fig. S1†). However, it was found that the annealing temperature was a key factor influencing the catalytic properties.59–61 In the present study, the as-prepared material was annealed at 450 °C for 2 h in Ar/H2 (100 sccm), resulting in the creation of a heterointerface made of cobalt molybdenum suboxides.
The crystal structure of the samples was characterized by X-ray diffraction (XRD). The XRD results confirm the formation of the CoMoO4 structure of the sample prepared via the microwave route (before annealing), as shown in Fig. S1† (JCPDS no. 15-0439). The XRD patterns of the annealed samples showed distinct diffraction peaks reflecting varying phase structures. XRD patterns of CMO-2 and CMO-1.5 exhibit peaks of Co2Mo3O8 (JCPDS no. 34-0511) suboxide phase (Fig. 1c and Fig. S2†), wherein the peak at 44.2° corresponds to metallic (111) plane of Co (JCPDS no. 15-0806). The diffraction peaks of the CMO-1 and CMO-1.25 could be indexed to a mixture of nanocrystalline Co2Mo3O8 and CoMoO3 phases along with CoO phase (Fig. S3†). The peaks observed at 36.7°, 42.6° and 61.9° correspond to CoO (JCPDS no. 01-75-0418) and the rest of peaks are attributed to the diffraction peaks of CoMoO3 or Co2Mo3O8, as marked in the plot. A detailed comparison of the XRD results of all the samples are presented in Fig. S2 and S3.†
The morphology of as-prepared sample was investigated by scanning electron microscopy (SEM). The SEM image of as-synthesized CMO-1.25 showed a well-aligned nanoplate morphology with lateral dimensions of 2 μm forming a flower-like morphology, densely covering the NF surface (Fig. 1d). The inset shows the EDX spectrum collected from the CMO-1.25, clearly revealing the presence of constituent elements. The morphology of the samples with varying compositions of Co/Mo does not seem to have changed upon annealing (Fig. S4†).
The EDX mapping images of CMO-1.25 shows an atomically uniform distribution of the Co, Mo and O after annealing (Fig. S5†). Transmission electron microscopy (TEM) images provided a thorough depiction of the sample. The sample scraped from the NF was sonicated in IPA, and a very dilute solution was drop-casted on the carbon-coated copper grids for the TEM study. A few micron-sized sheets (lateral dimension) made of closely packed nanoparticles were observed in the TEM image of CMO-1.25 (Fig. 1e).
Further analysis of the sample using high-resolution TEM (HR-TEM) and selected area electron diffraction (SAED) revealed that these sheets were composed of nanoparticles exhibiting various phases of cobalt molybdenum suboxide (Fig. 1f). While the HR-TEM image of CMO-1.25 clearly shows the presence of a heterointerface formed from cobalt molybdenum suboxide phases, Co2Mo3O8, CoMoO3, and CoO (Fig. 1f), CMO-2 was seen to exhibit Co2Mo3O8 phase alone, as revealed from the d spacing of 0.249 nm and 0.354 nm that correspond to (200) and (102) planes, respectively, which is consistent with the XRD findings (Fig. S6†). Another intriguing observation from the TEM studies is that the annealed samples are highly porous, which might have resulted from the loss of oxygen atoms during the reduction process (Fig. S7†).55 Such porous morphology favours improved ion diffusion, increases the catalytic activity towards HER and OER, and the charge transfer ability.62
We further performed X-ray photoelectron spectroscopy (XPS) studies to ascertain the phase and chemical state of the materials (Fig. 2 and Fig. S8†). The high resolution XPS spectra for the CMO-1.25 are shown in Fig. 2. All the spectra were calibrated with the binding energy of the C–C component at 284.8 eV. The XPS spectra of the as-prepared material obtained via microwave-assisted method show peaks corresponding to Co2+ and Mo6+, indicating a single-phase CoMoO4, which is in complete agreement with the XRD analysis. The microwave synthesized sample has cobalt in a Co2+ state, with peak positions at 796.0 and 780.4 eV corresponding to 2p1/2 and 2p3/2, respectively, with a peak separation of 15.6 eV (Fig. 2a). For the annealed sample, Co 2p XPS spectra show a pair of peaks corresponding to 2p1/2 and 2p3/2 with a separation of 15.7 eV and a pair of weak satellite doublet peaks (Fig. 2c). The characteristic peaks observed at binding energies of 795.8 and 780.1 eV are identified as Co2+ species,63,64 whereas the other two peaks at 801.5 and 785.0 eV are the satellite peaks ascribed to the Co2+ ions.65 Analysis of the Mo 3d spectrum for as-prepared CMO-1.25 shows the Mo6+ state corresponding to the CoMoO4 phase (Fig. 2b). Interestingly, the XPS spectra recorded for the annealed CMO-1.25 exhibit mixed oxidation states for molybdenum like Mo4+, Mo5+ and Mo6+ (Fig. 2d). The peaks observed at binding energies of 232.6 eV and 229.4 eV correspond to Mo4+, 233.7 eV and 230.4 eV correspond to Mo5+, and 235.4 eV and 232.3 eV correspond to Mo6+ oxidation states, which are the oxidation products of Mo species.66,67 Further, the O 1s XPS spectra was recorded, which showed peaks at ∼531.1 and ∼530.1 eV, corresponding to the lattice oxygen and the bonding state of Mo–O or Co–O, respectively (Fig. S8c, g and k†).68 The complete set of data recorded from the XPS analysis for all the studied Co/Mo composition are tabulated (Table S1, ESI†), and the corresponding high resolution spectra for all the annealed samples are shown in Fig. S8.† The inductively coupled plasma optical emission spectroscopy (ICP-OES) studies carried out for CMO-1, CMO-1.25, CMO-1.5, and CMO-2 showed a Co/Mo ratio of 0.97, 1.24, 1.65 and 1.8, respectively (Table S2†).
![]() | ||
| Fig. 2 XPS spectra of (a) Co 2p and (b) Mo 3d of CMO-1.25 before annealing, (c) Co 2p and (d) Mo 3d of CMO-1.25 after annealing. | ||
To gain insights into the reaction kinetics and investigate the influence of the overpotential on the steady-state current densities, corresponding Tafel plots were obtained from the respective LSVs (Fig. 3b). Tafel slopes and the exchange current densities are calculated from the Tafel equation (η = a + b
log
j) by plotting the overpotential (η) as a function of log
|j|.70 The smaller Tafel slope implies faster electron-transfer kinetics. The obtained Tafel slope of 63 mV dec−1 for the CMO-1.25 further confirms the excellent HER activity of the catalyst, compared with the other CMO catalysts with different Co/Mo molar concentrations. The overall electrocatalytic activity of CMO-1.25 is among the top level of reported non-precious alkaline HER catalysts (Fig. S9†). From the measured Tafel slope, the alkaline HER over the CMO-1.25 is believed to follow the Volmer–Tafel mechanism, and the Tafel step is the rate-determining step.59 We further measured the charge transfer resistance (Rct) of the catalysts using electrochemical impedance spectroscopy (EIS) technique and evaluated their electrochemical surface area using the CV method.
The uncompensated ionic and ohmic resistance of the electrochemical measurement system and the Rct of a catalyst are obtained from the EIS Nyquist plots.71Rct is related to the interface charge-transfer process of an electrode, and a smaller Rct value suggests a faster reaction rate, improved conductivity, which can drastically enhance the performance of the catalyst in the HER. As shown in Fig. 3c, CMO-1.25 was shown to exhibit an Rct of 11.2 Ω, which was lower than that of the other CMO samples (16.6 Ω, 22.6 Ω and 14.1 Ω for CMO-1, CMO-1.5 and CMO-2 respectively). The EIS data corroborate with the results obtained from the LSV curves and the Tafel slopes, confirming the superior electrocatalytic activity of CMO-1.25. Fig. 3d compares the overpotential and Tafel slope for the studied samples. We measured the double-layer capacitance (Cdl) in a non-faradaic potential region to assess the electrochemical active surface area of the catalysts. Fig. S10† compares the double-layer capacitances to indicate the change in ECSA for different samples at different scan rates of 10 mV s−1 to 100 mV s−1 in 1 M KOH solution. The ECSA of the catalysts is a critical parameter in evaluating their catalytic activity since a higher ECSA usually means more exposed active sites. Cdl, which is calculated from CV method, is proportional to the ECSA of the catalysts. The Cdl for CMO-1.25 catalysts is calculated to be ∼30 mF cm−2 while CMO-1 has 22.7 mF cm−2, CMO-1.5 has 20.9 mF cm−2 and CMO-2 has 22.1 mF cm−2. The phase-regulated growth of CoO/CoMoO3/Co2Mo3O8 nanoflakes could have resulted in the higher ECSA for the CMO-1.25 catalyst. The formation of defective structure of Co2Mo3O8 resulting from the in situ partial reduction of CoMoO4, as well as the presence of oxygen vacancies, is also believed to have contributed to higher ECSA.55 Fig. S11a† shows the LSV curves for HER, which are normalised by ECSA. The reductive annealing of CoMoO4 in an Ar/H2 atmosphere, seems to have changed the valence state of Mo. Meanwhile, the coordination of electrons in the chemical bonds of Co–Mo–O was changed, and the resulting oxygen vacancy rate was increased, as shown in the XPS results. It is to be noted that the oxygen vacancy plays a significant role in increasing the conductivity, electrochemically active sites and surface reactivity of the catalyst.72 Hence, the enhanced HER activity obtained for the CMO-1.25 sample would have resulted from the high oxygen vacancy ratio and its phase regulated interface with CoO/CoMoO3/Co2Mo3O8 hetero-structure phases.
The stability of the CMO-1.25 sample was further tested using chronopotentiometry and cyclic voltammetry (CV) methods, and the HER activity of the catalyst showed no significant change in its performance even after long cycling (6000 cycles) measurements (Fig. 3e). The catalyst exhibited a slight overpotential fluctuation of ±1 mV at a cathodic current density of 10 mA cm−2 over 10 h and an overpotential increase of only ±3 mV in the following 10 h of constant-current measurement performed at 100 mA cm−2 (Fig. 3f).
To explore the suitability of the studied catalysts for overall water splitting process, the OER activity of CMO-1, CMO-1.25, CMO-1.5 and CMO-2 catalysts grown on NF are investigated, and the corresponding polarization curves are shown in Fig. 4a. It can be seen that CMO-1.25 exhibits a much lower overpotential than other CMO catalysts. Further, the Tafel slope of CMO-1.25 is much lower (69 mV dec−1), suggesting its favourable OER kinetics (Fig. 4b). The electrocatalytic OER activity of CMO-1.25 with heterointerfaces is comparable to several of the previously reported Co–Mo compounds (Fig. S12†). EIS analysis was conducted to reveal more electrode kinetics information of the catalysts. The Nyquist plots in Fig. 4c shows that the Rct of CMO-1.25 catalyst is lower than the other CMO catalysts (Rct values, 25.8 Ω, 19.4 Ω, 24.9 Ω and 20.9 Ω are obtained for CMO-1, CMO-1.25, CMO-1.5 and CMO-2, respectively). The overpotential corresponding to 10 mA cm−2 and 100 mA cm−2 and the obtained Tafel slopes of different CMO catalysts are compared in Fig. 4d. CV method is used to calculate the Cdl, which are proportional to the ECSA of the catalysts (Fig. S13†). The CMO-1.25 shows a double layer capacitance of 28.4 mF cm−2, which is much larger than those of CMO-1 (25.9 mF cm−2), CMO-1.5 (20.8 mF cm−2) and CMO-2 (22.5 mF cm−2). The high Cdl of CMO-1.25 suggests enhanced catalytically active surface sites for the reaction. The results shown in Fig. S11b† indicate that CMO-1.25 shows much improved OER activity compared to other CMO catalysts studied, reflecting that the enhanced OER activity of the sample is attributed not only to the increased ECSA but also the improved intrinsic activity of the catalyst due to the optimised heterointerface structure. Further, we studied the durability of the catalysts for OER and was found that the OER activity of CMO-1.25 showed only a slight decay (±20 mV) over 6000 CV cycles (Fig. 4e). The constant-current tests (10 h) also showed much improved electrochemical performance of CMO-1.25 catalyst, at anodic current densities of 10 and 100 mA cm−2 (Fig. 4f). Even at a larger current density of 100 mA cm−2, the CMO-1.25 electrode exhibited only 6 mV increase in the overpotential, retaining 98% of its initial catalytic activity after 10 h. The obtained results clearly show excellent bi-functional electrocatalytic activity of CMO-1.25 for alkaline HER and OER, suggesting their suitability as potential electrode materials for overall water splitting.
We also fabricated an anion exchange membrane electrolyser using the bifunctional CMO-1.25 catalyst to evaluate its practical applicability in overall water splitting (Fig. 5d). The schematic of the electrolyser setup is shown as inset of Fig. 5e. The reactor consists of an anion exchange membrane (Fumasep, FAS 50) at the middle, two gaskets on its sides, and with two 1.7 × 1.7 cm electrodes (using CMO-1.25 electrocatalyst) for HER and OER. Two polar plates are connected at the end. The FAS membrane was activated in 1 M KOH for 24 h before the experiment and used as such for the experiments. Throughout the experiment, a constant electrolyte flow (1 M KOH) was maintained in the reactor at 60 °C. The potentio-dynamic polarization curve recorded for the electrolyser with CMO-1.25 as HER and OER electrocatalysts are shown in Fig. S16a† and Fig. 5e. The experiment is done by holding at a different potential, from 1.3 V to 2.1 V, for 60 s. The obtained polarization curves show that at 1.5 V the cell delivers a current density of 126 mA cm−2.
The cell shows a very low current density at 1.3 V (23 mA cm−2), and the current obtained from the electrolyser increased exponentially with voltage and reached to almost constant value after 2 V (781 mA cm−2). The current findings are superior to several of the similar reported studies.60,74,75,78–81
As compared to industrial alkaline water electrolyser, which require 1.7 to 2.4 V to reach 300 mA cm−2 at 60–90 °C, the present cell delivers a current density of 350 mA cm−2 at 1.7 V. This clearly shows the high energy efficiency of the reactor with CMO-1.25 bifunctional electrocatalysts for overall water splitting.82 The performance of the fabricated electrolyser reactor is compared with the previously reported studies (Table S4†). The amount of hydrogen generated at different voltages was measured using an inverted burette (displacement method), and the obtained values are given in Fig. 5e and Fig. S16b.† As shown in Fig. S16b,† the calculated amount of hydrogen generated by the displacement method (experimentally) is in correlation with the calculated values using Columbic method (theoretical), except that there is a slight variation in the high current density region. Moreover, the amount of hydrogen generated at 1.8 V is measured to be ∼ 11–12 mL min−1, i.e., with 85–95% coulombic efficiency. The long-term stability of the device was studied at constant operating potentials of 1.6 V and 1.8 V (Fig. 5f). The cell gives a current density of 220 mA cm−2 @1.6 V and 670 mA cm−2 @1.8 V. The device showed very good long-term durability and retains a stable performance with 95% of its activity at 1.6 V and 1.8 V over 12 h. The present work clearly shows that the CMO-1.25 electrocatalyst exhibits excellent stability and activity for overall water splitting and has full potential for industrial implementation towards large scale hydrogen production. The impressive bifunctional electrocatalytic activity of the material is resulted from the synergistic effect of the heterointerface formed by the cobalt molybdenum suboxides.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3nr02458j |
| This journal is © The Royal Society of Chemistry 2023 |