Akerke Bereketovaa,
Muthuchamy Nallal*ab,
Mohammad Yusufa,
Sanha Janga,
Karthick Selvamc and
Kang Hyun Park*a
aDepartment of Chemistry, Pusan National University, Busan 46241, Republic of Korea. E-mail: chemistry@pusan.ac.kr; muthu@szu.edu.cn; nm2020mnature@gmail.com
bCollege of Physics and Optoelectronic Engineering, Shenzhen University, 1066 Xueyuan Avenue, Nanshan District, Shenzhen, 518060, China
cNano & Computational Materials Lab, Department of Industrial Chemistry, Alagappa University, Karaikudi 630003, Tamilnadu, India
First published on 7th May 2021
In this study, we constructed a highly effective, low-cost, non-noble-metal-based electrocatalyst to replace Pt catalysts, with a CoS@SNC catalyst being successfully synthesized. The obtained nanocatalyst was characterized via scanning electron microscopy, energy-dispersive X-ray spectroscopy, transmission electron microscopy, powder X-ray diffraction studies, and X-ray photoelectron spectroscopy. Herein, an initially prepared N-containing Co MOF formed flower-like particles, which were obtained via a solvothermal method; further it was used for a sulfuration process as a template to achieve an S,N (heteroatom)-doped carbon electrocatalyst with embedded CoS (CoS@SNC). The synthesized flower-like CoS@SNC electrocatalyst derived from a novel MOF showed a uniform distribution of Co, S, N, and C at the molecular level in the MOF and it was rich in active sites, facilitating enhanced electrocatalytic performance. During the HER and OER in 0.1 M KOH solution, to reach a current density of 10 mA cm−2, lower overpotentials of −65 mV and 265 mV, respectively, were required and Tafel slopes of 47 mV dec−1 and 59.8 mV dec−1, respectively, were seen. In addition, due to a synergistic effect between CoS and the S,N-doped carbon matrix, long-term durability and stability were obtained. This facile synthetic strategy, which is also environmentally favorable, produces a promising bifunctional electrocatalyst.
In the past decade, as alternatives to noble metals for HER and OER applications, heteroatom-doped porous carbon hybrid matrices have been investigated and have stimulated a great deal of interest because of their cost-effectiveness, large numbers of accessible active sites, and high conductivity.9,10 In particular, dual heteroatom-doped carbon-based materials with the encapsulation of transition metals (such as Ni, Fe, and Co) or derivative compounds have shown high activity during electrocatalysis, benefiting from synergistic effects, stability, and large numbers of active sites.11–13 Among transition metal catalysts, Co-based electrocatalysts, which are located near the top of bifunctional water-splitting “volcano plots”, may be highly promising candidates to act as outstanding water oxidation catalysts.14,15 In addition, Co–carbon matrices that are obtained via an annealing process show unique interactions between the metal and carbon materials, demonstrating high durability and high electrical conductivity for the OER and HER.16 Notably, a pyrite-type sulfur- and nitrogen-doped electrocatalyst (CoSx/S,N-co doped CNTs) exhibited exceptionally superior bifunctional OER/ORR catalytic activity, with a ΔE (ΔE = E10 − E1/2) value of ∼0.760 V. The study of this material revealed that a heteroatom decoration strategy enhances the electrocatalytic activity and also accelerates the reaction kinetics, whereas CoS nanocrystals are protected by a robust and chemically stable carbon matrix, avoiding the self-accumulation of catalytically active sites and resulting in increased long-term durability.17 In the same way, Co@N,S-doped CNTs exhibited excellent electrocatalytic HER activity, which was attributed to a synergistic effect between N/S atoms, the rich active sites of the Co nanoparticles, and structural defects/edges from the carbon matrix.18
Accordingly, developing synthesis strategies for multicomponent materials with novel morphologies can provide more active sites, good stability, and desirable electrocatalytic properties.19,20 Many studies have established that metal–organic frameworks (MOFs) derived from metal ions and organic ligands are an attractive and promising type of precursor for catalyst preparation as a result of their large surface areas and well-defined structures.21–23 In particular, MOFs derived from N-containing ligands have been considered as favorable templates for obtaining N-doped carbon-based materials that have further been utilized as low-cost effective electrocatalysts.24,25 Moreover, additional (S,P) heteroatom doping into N-containing MOFs at high temperatures (such as via phosphorization and sulfuration processes) is a non-precious-metal-based strategy leading to the uniform scattering of metals and the controlled doping of selected heteroatoms. As a result, catalytic activity can be enhanced due to the formation of porous structures with more active sites and high conductivity, resulting in good bifunctional electrocatalytic performance.26–29
Herein, based on the abovementioned considerations, a novel flower-like electrocatalyst has been designed, which consists of cobalt sulfide embedded in S,N (heteroatom)-codoped carbon (CoS@SNC); a prepared Co MOF with dual organic ligands (btec: 1,2,4,5-benzenetetracarboxylate; and ted; triethylenediamine) was used as a precursor for sulfuration. The Co MOF derived from C-abundant H4btec and N-loaded ted was synthesized via an in situ solvothermal method. A sulfuration process at high temperature has been adopted in order to create CoS@SNC with uniformly distributed metal sulfides and S,N heteroatom doping in the carbon matrix. Well-distributed CoS particles and N,S heteroatom doping in the carbon shell provided a mesoporous structure and abundant catalytically active sites, which were favorable for increasing the electrocatalytic properties. The electrochemical activity of CoS@SNC was tested with respect to its HER and OER performances. The results showed that CoS@SNC presents efficient bifunctional activity toward both the HER and OER with low overpotentials of −65 mV and 265 mV, respectively, and Tafel slopes of 47 mV dec−1 and 59.8 mV dec−1, respectively, in 0.1 M KOH solution. In this work, the experimental results suggest that a facile and inexpensive bifunctional HER and OER electrocatalyst has been developed.
The potential observed versus the Ag/AgCl electrode was converted to RHE according to the following equation: ERHE = EAg/AgCl + 0.197 + 0.059 pH. For comparison, commercial Pt20%@C was coated on a GCE and the HER and OER performances were studied. Time-dependent current density measurements at a constant overpotential (V vs. RHE) were performed to test the stability of the catalyst. Electrochemical impedance spectroscopy (EIS) was performed over a frequency range from 100 kHz to 100 Hz. The turnover frequency (TOF) was calculated from the current density. The formula for TOF calculations was TOF = (jA)/(4Fn),31 where j is the current density (mA cm−2) at a given point; A is the surface area of the working electrode; 4 is the electron transfer number during oxygen (O2) gas production; F is the Faraday constant (F = 96485 C mol−1); and n is the number of moles of active material. It is assumed that Co in CoS@SNC is active and contributes to the bifunctional electrocatalytic reaction, so n is the Co ion molar number.
Scheme 1 A schematic illustration of the synthesis process of CoS@SNC and the chemical structure of the synthesized Co MOF. |
The morphology and size of CoS@SNC were studied using scanning electron microscopy (SEM) and transmission electron microscopy (TEM). As can be seen from SEM images (Fig. 1a and b), the novel Co MOF particles were composed mainly of flower-like particles with smooth surfaces. Fig. 1c and d shows CoS@SNC after the sulfuration process, wherein the morphology can be compared with what is seen in Fig. 1a and b, without particular shape changes; however, the surface demonstrates a barely visible additional layer, which demonstrates the successful sulfuration of the as-prepared Co MOF precursor and that the carbon hybrid matrix was maintained. The average width and length of the synthesized flower-like CoS@SNC catalyst was around 150 nm and 1 μm, respectively. To collect clear characterization data relating to the microstructure and particle distribution, TEM and HRTEM images were also obtained. In the semitransparent morphology of CoS@SNC (Fig. 2a and b), the obvious dark spaces indicate homogeneously distributed CoS nanoparticles, whereas the gray spaces represent the carbon hybrid matrix. A HRTEM image (Fig. 2c) taken from a selected area of a CoS@SNC nanoparticle reveals interplanar distances of 0.193 nm (1.93 Å) and 0.292 nm (2.92 Å), corresponding to the (102) and (100) lattice planes of CoS, respectively. In addition, after size measurements, small CoS particles with a diameter of around 7 nm were found (Fig. 2d). High-angle annular dark field scanning transmission electron microscopy (HAADF-STEM) and energy-dispersive X-ray spectroscopy mapping images, as displayed in Fig. 3a and b–e, respectively, present a uniform distribution of Co, S, N, and C elements in the selected range. Herein, the obtained N and S co-doped carbon is favorable for enhancing the electrical conductivity and catalytic activity of the carbon hybrid matrix.32
Fig. 1 (a) and (c) Low- and (b) and (d) high-magnification SEM images of (a)–(b) Co MOF and (c)–(d) CoS@SNC. |
Fig. 2 (a) and (b) TEM and (c) HRTEM images of CoS@SNC (inset of (c): the SAED pattern). (d) The size distribution diagram of CoS particles corresponding to TEM image data. |
Fig. 4 displays the typical X-ray diffraction (XRD) patterns of the Co MOF precursor (red curve) and CoS@SNC (blue curve). After the sulfuration of the Co MOF precursor, the obtained diffraction peaks of CoS@SNC can be indexed to the CoS crystal phase (JCPDS card no. 19-0366), which implied successful conversion into CoS at high temperature.33 The surface area and porosity of synthesized CoS@SNC were evaluated via N2 adsorption–desorption experiments. Fig. 5 shows a type-IV isotherm with a distinct hysteresis loop, indicating the presence of mesoporous structures in the sample. The obtained surface area for CoS@SNC is 51.7 m2 g−1. The corresponding pore size distribution calculated using the Barrett–Joyner–Halenda (BJH) method (Fig. 5, inset) indicates the presence of mesoporous structures with the pore diameter concentrated at approximately 13.3 nm. Meanwhile, the pore volume of CoS@SNC is 0.142 cm3 g−1. CoS@SNC with massive mesopores would be beneficial for mass and charge transfer when applied to electrocatalysts.34 The thermal stabilities of the synthesized Co MOF and CoS@SNC were explored via TGA (Fig. S1†). The synthesized materials were heated from 25 °C to 600 °C at a rate of 10 °C min−1 under a nitrogen atmosphere. Both Co MOF and CoS@SNC presented gradual weight loss at ∼120 °C, corresponding to the removal of adsorbed guest molecules on the surfaces. Co MOF shows three major weight-loss steps in the range between 230 °C and 580 °C, which may correspond to the decomposition of organic ligands. Comparatively, CoS@SNC shows higher thermostability than Co MOF at a temperature of 600 °C, showing only 29% weight loss compared with 84% weight loss for Co MOF.
Fig. 5 The N2 adsorption–desorption isotherm of CoS@SNC (inset: the corresponding pore size distribution). |
Furthermore, X-ray photoelectron spectroscopy (XPS) measurements were carried out to estimate the chemical composition and elemental valence states of CoS@SNC. The full spectrum, as shown in Fig. 6a, confirms the existence of Co, C, S, N, and O elements in CoS@SNC. Narrow scans of the chemical states of elements were evaluated, focusing on Co 2p, C 1s, S 2p, and N 1s. The Co 2p spectrum (Fig. 6b) can be resolved into two spin–orbit doublets and two satellite peaks. The peak with a binding energy of 778.30 eV with a Co 2p3/2 satellite peak corresponds to the orbital characteristics of Co2+ in CoS@SNC. The C 1s spectrum exhibits 3 peaks with binding energies of about 284.50 eV (C–C), 285.70 eV (C–S, C–N, C–O), and 288.33 eV (C–OC). The observed peaks related to C–N and C–S confirm the substitution of N and S atoms. Moreover, they correspond to successful S-atom doping into the carbon matrix after the sulfuration process. As shown in Fig. 6d, the N 1s spectrum displays the presence of pyrrolic N, pyridinic N, and graphitic N at binding energies of 398.76 eV (33.43%), 400.01 eV (49.31%), and 401.87 eV (17.27%), respectively. The existence of N atoms comes from using N-loaded organic ligands (triethylenediamine) in the synthesis of Co MOF. Meanwhile, the presence of pyridinic N and graphitic N are suggested to support enhanced HER and OER catalytic activity. The S 2p spectrum peaks (Fig. 6e) with binding energies of 162.38 eV and 163.30 eV are attributed to the S 2p3/2 and S 2p1/2 orbitals of CoS, respectively. The other two peaks at 163.65 eV and 164.63 eV can be assigned to C–S S 2p3/2 and S 2p1/2.35,36
Fig. 6 XPS high-resolution spectra of CoS@SNC: (a) full spectrum, and (b) Co 2p, (c) C 1s, (d) N 1s, and (e) S 2p spectra. |
The electrocatalytic behaviors of CoS@NC and Co MOF were investigated in N2-saturated 0.1 M KOH solution using cyclic voltammetry (Fig. 7). CV plots for CoS@SNC (Fig. 7a) and Co MOF (Fig. 7b) were obtained upon the variation of the potential from 0.82–1.6 V vs. RHE in 0.1 M KOH solution. In alkaline media, CoS electrode redox can take place between different valence states (Co2+, Co3+, and Co4+).37 Fig. 7a shows a large cathodic redox peak and two anodic oxidation peaks, corresponding to the following reactions:
CoS + OH− ↔ CoSOH + e− | (1) |
CoSOH + OH− ↔ CoSO + H2O + e− | (2) |
Fig. 7 Cyclic voltammetry plots of (a) CoS@SNC and (b) Co MOF electrodes at a scan rate of 10 mV s−1 over the voltage range of 0.82–1.6 V vs. RHE in 0.1 M KOH. |
Electrochemical impedance spectroscopy studies were carried out (Fig. 8) using both CoS@SNC and Co MOF electrodes in the frequency range of 100 kHz to 100 Hz in 0.1 M KOH. The corresponding Nyquist plot of CoS@SNC shows a lower charge transfer resistance (6 Ω) than that of Co MOF (7 Ω). The determined value indicates the better electron transfer properties of CoS@SNC, suggesting the positive effects of the sulfuration of Co MOF. The lower charge transfer resistance value could provide faster charge transfer and more favorable kinetics for the OER and HER.38,39
Fig. 8 Electrochemical impedance spectra with the equivalent Randles circuit for CoS@SNC and Co MOF electrodes over the frequency range of 100 kHz to 100 Hz in 0.1 M KOH. |
The electrocatalytic performance of CoS@SNC for the OER was studied in 0.1 M KOH solution. To obtain meaningful comparisons, the CoS@SNC catalyst was also tested with the Co MOF precursor and commercial Pt20%@C. As shown in Fig. 9, the corresponding polarization curves of the samples were measured via linear sweep voltammetry (LSV) at a scan rate of 10 mV s−1. To achieve a current density of 10 mA cm−2, the CoS@SNC catalyst exhibits the lowest overpotential of 265 mV (Fig. 9a), lower than those of Co MOF (311 mV) and Pt20%@C (464 mV). Fig. 9b shows the calculated Tafel plots of all investigated samples. The corresponding Tafel slope value for the CoS@SNC catalyst is 59.8 mV dec−1, which is even better than the Co MOF precursor (63.3 mV dec−1) and commercial Pt20%@C (69.7 mV dec−1). The Tafel slope provides information about the kinetics of the electrocatalyst during the OER reaction; subsequently, a lower Tafel slope means greater catalytic activity for the OER. As can be seen in Fig. 9c, a comparison of the determined potentials and Tafel slopes indicates that CoS@SNC (CoS@SNC > Co MOF > Pt20%@C) has good kinetics that are preferable for the OER. Overall, the CoS@SNC catalyst shows much better electrocatalytic activity towards the OER with an overpotential of 265 mV and a Tafel slope value of 59.8 mV dec−1, which are smaller than the values for other Co-based catalysts (Table S1†).
The TOF of CoS@SNC is calculated to be 8.38 × 10−1 s−1 at an overpotential of 300 mV, which is among the best TOF values for Co-based electrocatalysts in recent reports.40–42 Fig. 10a displays the stability test results for the CoS@SNC catalyst after 5000 cycles. The obtained polarization curve demonstrates that even after 5000 cycles, the initial onset potential of CoS@SNC is still stable, without shifting. Also, when the morphology of CoS@SNC was observed after stability testing for 5000 cycles, it was not distorted and remained intact (Fig. S1†), indicating the excellent stability of the CoS@SNC electrocatalyst. Furthermore, chronoamperometric durability testing (Fig. 10b) of CoS@SNC was carried out at a constant overpotential voltage of 1.54 V in 0.1 M KOH solution at a scan rate of 10 mV s−1. In this case, it was evaluated that CoS@SNC showed long-lasting durability for over 10000 s. The inset image shows peaks from the destruction and formation of O2 gas bubbles, which supports the existence of the OER.
Fig. 10 (a) Polarization curves collected before and after the stability testing of CoS@SNC towards the OER. (b) Chronoamperometric durability testing at 1.54 V. |
The kinetics of the HER performance were examined for Co@SNC in 0.1 M KOH solution. As shown in Fig. 11a, the onset potentials are 18.9 mV, −45.3 mV, and −13.9 mV and the overpotentials are −65 mV, −309 mV, and −19 mV for CoS@SNC, Co MOF, and Pt20%@C, respectively, at a current density of 10 mA cm−2. The Tafel slope (Fig. 11b) calculated from the LSV curve for the CoS@SNC catalyst is approximately 47 mV dec−1, which is considerably smaller than the value for Co MOF (63 mV dec−1) and close to commercial Pt20%@C (28 mV dec−1). Conforming to classical theory, different Tafel slope values correspond to different reaction mechanisms of hydrogen evolution. First is the Volmer reaction, where proton adsorption occurs with a high Tafel slope of ∼120 mV dec−1, and second is the Heyrovsky or Tafel reaction, which indicates molecular hydrogen evolution with a low Tafel slope of ∼40 mV dec−1 or ∼30 mV dec−1, respectively. The lower Tafel slope of the CoS@SNC catalyst indicates that the HER involves a Volmer–Heyrovsky reaction. A comparison of the determined potentials and Tafel slopes also displays the enhancement of the catalytic activity of CoS@SNC over Co MOF for the HER performance. Moreover, the CoS@SNC electrocatalyst exhibits excellent electrochemical performance (overpotential = −65 mV and Tafel slope = 47 mV dec−1) compared with other recently reported HER electrocatalysts (Table S2†).
For well-studied cobalt-based bifunctional electrocatalysts, it is commonly known that a high valence state of Co is critical for obtaining bifunctional water-splitting performance because its availability can enhance the electrophilicity of Oad, thus facilitating the formation of OOHad via an incoming hydroxide anion and oxygen atom being associated with Co cations. As shown in Fig. 7, before the steep rise in the CV curve of CoS@SNC in 0.1 M KOH alkaline medium, the slope of CoS is higher than that of Co(OH)2 in Co MOF, which means that many Co cations are present on the CoS surface before the OER process. Additionally, the improved electroconductivity, porous environment, including nanopores, and the availability of N, S, and C on CoS@SNC can offer a favorable microenvironment at the interface between Co and the electrolyte to trigger the OER and HER processes, as mentioned above. The Co-MOF-derived and S-heteroatom-doped CoS@SNC catalyst can thus show synergistically boosted bifunctional performance to achieve excellent OER and HER catalytic activities.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1ra01883c |
This journal is © The Royal Society of Chemistry 2021 |