Anqi
Ju
b,
Shuxian
Zhang
b,
Dong
Li
b,
Kunming
Li
b,
Xuepeng
Ni
b,
Yi
Li
a and
Yang
Jiang
*a
aNanotechnology Research Institute & College of Materials and Textile Engineering of Jiaxing University, Jiaxing City 314001, Zhejiang Province, P. R. China
bState Key Laboratory for Modification of Chemical Fibers and Polymer Materials & College of Materials Science and Engineering, Donghua University, Shanghai 201620, China
First published on 4th December 2023
Owing to the clean and environment friendly advantages, electrochemical water splitting stands out among various hydrogen production strategies. Electrocatalysts play an important role in the hydrogen evolution reaction (HER). Hence, Pt-(Ni0.5Co0.5)2P/S-carbon fibers as electrocatalysts for highly efficient HER were prepared through the structural designing of CNF and heteroatom doping (sulfur (S) or boron (B)). First, three composites of the (Ni0.5Co0.5)2P/carbon fiber ((Ni0.5Co0.5)2P/CNF), (Ni0.5Co0.5)2P/porous carbon fiber ((Ni0.5Co0.5)2P/PCNF), and (Ni0.5Co0.5)2P/hollow porous carbon fiber ((Ni0.5Co0.5)2P/HPCNF) were fabricated via a facile electrospinning with a solvothermal method. (Ni0.5Co0.5)2P/PCNFs showed the smallest overpotential at a current density of 10 mA cm−2 among the three structures. (Ni0.5Co0.5)2P nanosheets loaded on the porous CNF with a large active surface area may expose active sites and shorten the ion transport channel. To improve the catalytic performance of (Ni0.5Co0.5)2P/PCNF, Pt nanoparticles were anchored on (Ni0.5Co0.5)2P/heteroatom doped-PCNF by the chemical reduction method. Pt-(Ni0.5Co0.5)2P/S doped-PCNF exhibited a small overpotential of 64 mV for the HER with 74.9 mV dec−1 Tafel slope and a good stability, which was attributed to the conductive S-doped PCNF facilitating electron transport, accompanying the synergistic effect between the bimetallic phosphide and Pt nanoparticles, thus providing a facile method for an efficient HER electrocatalysis.
In this study, Pt nanoparticles-anchored-(Ni0.5Co0.5)2P/heteroatoms doped-carbon nanofibers, as electrocatalysts for efficient HER, were prepared by electrospinning, solvothermal method, and chemical reduction. Firstly, three kinds of CNF with different structures (CNF, PCNF, HPCNF) were designed as substrates for (Ni0.5Co0.5)2P. (Ni0.5Co0.5)2P/PCNF exhibited the smallest overpotential (164 mV) due to the large active surface area and catalytic active sites. Secondly, Pt nanoparticles and (Ni0.5Co0.5)2P nanosheets were anchored on heteroatom-doped PCNF to promote the HER performance of (Ni0.5Co0.5)2P/PCNF, so that the prepared Pt-(Ni0.5Co0.5)2P/SPCNF may exhibit a small overpotential of 64 mV with a lower Tafel slope (74.9 mV dec−1) for HER at the current density of 10 mA cm−2 with good stability in alkaline electrolytes.
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1 (0.75
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0.25 mL h−1). The as-prepared carbon nanofibers were heated at 280 °C for 120 min in air for stabilization. Finally, the preoxidized nanofibers were carbonized at 800 °C for 120 min under a nitrogen atmosphere to obtain different structures of the carbon nanofibers.
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1 v/v) mixed solution, and then 15 μL of 5% Nafion solution was added to obtain a uniform catalyst ink. 6 μL of the above ink was loaded on a clean GCE (0.42 mg cm−2), and dried at 60 °C to prepare the working electrode. All the electrochemical tests were recorded on an electrochemical workstation (IVIUM). (1) The polarization curves of HER were recorded using linear sweep voltammetry (LSV) at a scan rate of 5 mV s−1, the voltage drop was manually compensated by Ecompensated = Emeasured − iRs, where Rs was obtained by EIS. Besides, all the measured potentials were converted into a reversible hydrogen electrode (ERHE = EHg/HgO + 0.098 + 0.059 × PH). (2) The electrochemical active area (ECSA) of the catalyst was calculated by the double-layer capacitance Cdl, which was measured by cyclic voltammetry (CV) in a non-faradaic potential region at different scan rates. (3) Electrochemical impedance spectroscopy (EIS) was performed with a frequency range from 105–10−1 Hz, and 5 mV of the amplitude. (4) The stability was tested from the continuous 2000 CV cycling at a scan rate of 100 mV s−1. Unless otherwise noted, the current density in the electrochemical test results was calculated based on the geometric area of the electrode. All data were measured using iR compensation.
The effect of the Ni/Co ratio in (NixCo1−x)2P on the morphology and electrochemical performance of (NixCo1−x)2P/CNF was studied and the data are shown in Fig. S1–S3 (ESI†). The surface of the carbon nanofiber was uniformly coated with (NixCo1−x)2OH nanosheets for all samples (Fig. S1, ESI†). After the in situ phosphidation, the morphology of (NixCo1−x)2P/CNF remained unchanged (Fig. S2, ESI†). The (Ni0.5Co0.5)2P/CNF composite displayed an overpotential of 179 mV, which was much smaller compared to others as shown in Fig. S3 (ESI†). Therefore, the Ni/Co molar ratio (0.5/0.5) was used in the following studies. The morphologies of (Ni0.5Co0.5)2P/CNF, (Ni0.5Co0.5)2P/PCNF and (Ni0.5Co0.5)2P/HPCNF are shown in Fig. 1a–c. The interconnected nanosheets were evenly distributed on the surface of the carbon fiber and a large number of active sites were introduced, which are vital to the electrocatalytic performance. Moreover, negatively charged P atoms act as proton acceptors, whereas, positively charged metal atoms act as hydride acceptors in NiCoP, both of which are crucial active sites.31,32 Meanwhile, compared to the transition metal oxides, TMPs showed good conductivity and could more effectively accelerate the charge transfer. The porous and hollow porous structures of PCNF and HPCNF are also shown in the insert of Fig. 1b and c. The SEM image of (Ni0.5Co0.5)2P/SPCNF is depicted in Fig. 1d. The diameter (1.5–2 μm) of the heteroatom-doped carbon fibers was significantly larger than that of the undoped carbon nanofibers (400–700 nm) and the Pt nanoparticles were evenly embedded on the surface of (Ni0.5Co0.5)2P/SPCNF. Similar results were also observed in the SEM of Pt-(Ni0.5Co0.5)2P/PCNF, Pt-(Ni0.5Co0.5)2P/BPCNF, and Pt-(Ni0.5Co0.5)2P/BSPCNF, as shown in Fig. S4 (ESI†).
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| Fig. 1 SEM images of (a) (Ni0.5Co0.5)2P/CNF, (b) (Ni0.5Co0.5)2P/PCNF, (c) (Ni0.5Co0.5)2P/HPCNF, and (d) Pt-(Ni0.5Co0.5)2P/SPCNF. | ||
Fig. 2a shows the transmission electron microscopy (TEM) images of (Ni0.5Co0.5)2P/PCNF, the 3D cross-linked (Ni0.5Co0.5)2P nanosheets were uniformly distributed on the surface of the porous carbon fibers, which was consistent with the SEM results. As shown in the high-resolution transmission microscope (HRTEM) image (Fig. 2b and c), the lattice spacings of 0.22 and 0.20 nm correspond to the (111) and (201) planes of NiCoP, respectively, indicating the successful preparation of bimetal phosphide. Furthermore, the elemental mapping images confirmed that Ni, Co, and P were evenly scattered on the porous carbon nanofibers, as shown in Fig. 2d. The TEM of Pt-(Ni0.5Co0.5)2P/BSPCNF is shown in Fig. S5 (ESI†). The (Ni0.5Co0.5)2P nanosheets were prepared and numerous Pt nanoparticles were distributed on the Pt-(Ni0.5Co0.5)2P/BSPCNF. Moreover, B and S elements could be detected from both elemental mapping and energy dispersive X-ray spectroscopy spectrum (Fig. S6, ESI†), indicating doping of B and S in CNF. All the above results confirmed the preparation of Pt-(Ni0.5Co0.5)2P/BSPCNF.
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| Fig. 2 (a) TEM and (b) and (c) HRTEM images of the prepared (Ni0.5Co0.5)2P/PCNF and (d) the corresponding element mapping of Ni, Co, P, and C. | ||
XRD analysis was carried out to further study the crystalline structure of the as-prepared composites. The results from the XRD patterns (Fig. 3a) showed that the carbon nanofibers showed a strong characteristic peak at around 26°, which belonged to the (002) crystal facets of graphitic carbon. However, new peaks were observed at 41.07°, 44.92°, 47.64°, and 54.71° for all the composites, which were ascribed to the (111), (201), (210), and (002) crystal planes of the NiCoP crystal phase (JCPDS no. 71-2336). The structure of the carbon fibers had no effect on the crystalline phase of NiCoP. Compared to the above, Pt-(Ni0.5Co0.5)2P/(X)PCNF showed other weak characteristic peaks at around 39.8° and 46.9°, as shown in Fig. S7 (ESI†), belonging to the (111) and (200) planes of the face-centered cubic Pt (JCPDS no. 04-0802), respectively. However, no obvious characteristic peaks of sulfur (S) and boron (B) were observed, mainly because of the small doping amounts. Besides, we also explored the crystalline structure of the composites prepared with different Ni/Co ratios. When there were different Ni/Co molar ratios, the XRD patterns displayed single metal phosphide or bimetallic phosphate characteristic peaks (Fig. S8, ESI†), which corresponded to Ni2P (JCPDS no. 03-0953), NiCoP33 (JCPDS no. 71-2336), and CoP (JCPDS no. 29-0497) phases. The Raman spectra of the composites (Fig. 3b), there were obvious D-band and G-band at 1347 cm−1 and 1590 cm−1, corresponding to the characteristic peaks of amorphous carbon and graphitized carbon, respectively, while the intensity ratios of D and G peaks were 0.951 for PCNF and 0.955 for (Ni0.5Co0.5)2P/PCNF. Similar values indicated that the crystal structure of the carbon fiber was not destroyed by hydrothermal and phosphidation.
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| Fig. 3 (a) Raman spectra of the PCNF and (Ni0.5Co0.5)2P/PCNF. (b) XRD patterns of the prepared (Ni0.5Co0.5)2P/CNF, (Ni0.5Co0.5)2P/PCNF, and (Ni0.5Co0.5)2P/HPCNF. | ||
The surface chemical composition of (Ni0.5Co0.5)2P/PCNF was characterized by X-ray photoelectron spectroscopy (XPS). The high-resolution spectra of C 1s, P 2p, Ni 2p, and Co 2p are displayed in Fig. 4a–d. The spectrum of C 1s possessed three characteristic peaks corresponding to the C–C bond (284.8 eV), C–O bond (286 eV), and C
C–O bond (288 eV), as shown in Fig. 4a. In the XPS spectrum of P 2p (Fig. 4b), the peaks at 129.1 and 130.2 eV resulted from P 2p3/2 and P 2p1/2, respectively, and one peak (P–O) was located at 133.5 eV, resulting from the material oxidation in air.34 The high-resolution XPS spectrum of Ni 2p showed peaks at different binding energies (Fig. 4c), the two main peaks could be assigned at 856.7 eV and 874.3 eV to Ni 2p3/2 and Ni 2p1/2, respectively, correspond to Ni-P in (Ni0.5Co0.5)2P/PCNF. The two satellite peaks at 864.2 eV and 880.8 eV corresponded to Ni 2p3/2 and Ni 2p1/2, respectively, in Ni–O. For the Co 2p spectrum shown in Fig. 4d, the peaks at 782.21 (Co 2p3/2) are ascribed to Coδ+ in the Co–P compound, and the Co 2p1/2 located at 798.07 eV could be attributed to the oxidized Co species in the Co–P compound.35 Two satellite peaks at 782.2 eV and 798.0 eV, and the peak at 776.75 eV belonged to the Co0+ species. The XPS spectrum of Pt-(Ni0.5Co0.5)2P/SPCNF was recorded and deconvoluted, as shown in Fig. S9 (ESI†). Compared to (Ni0.5Co0.5)2P/PCNF, the binding energy and valence states of Ni, Co, P, and C did not show any obvious changes. Three characteristic peaks appeared in the spectrum of Pt 4f (Fig. S9e, ESI†), the binding energies at 69.5 eV and 72.5 eV are characteristic peaks of Pt 4f7/2, and the binding energies at 74.9 eV and 76.4 eV are assigned to Pt 4f5/2. Due to the S-doping of PCNF, the new peaks appeared at 164.8 eV and 163.6 eV, corresponding to C–S and S–S, respectively (Fig. S9b, ESI†). Based on the above structural information, the preparation of NiCoP nanosheets was well demonstrated.
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| Fig. 4 High-resolution XPS spectra of (a) C 1s, (b) Co 2p, (c) Ni 2p, and (d) P 2p of the (Ni0.5Co0.5)2P/PCNF. | ||
The electrocatalytic performances of (Ni0.5Co0.5)2P/CNF, (Ni0.5Co0.5)2P/CNF (Ni0.5Co0.5)2P/PCNF, and (Ni0.5Co0.5)2P/HPCNF composites were measured by a tri-electrode system in 1M KOH solution to study the impact of the CNF structure. The LSV curves with a scan rate of 5 mV s−1 are shown in Fig. 5a. (Ni0.5Co0.5)2P/PCNF showed an overpotential of 164 mV for a current density of 10 mA cm−2. These results indicated that the HER activity of the (Ni0.5Co0.5)2P/PCNF was better than that of the (Ni0.5Co0.5)2P/CNF and (Ni0.5Co0.5)2P/HPCNF, implying that the PCNF with porous structure increased the contact area of the electrode/electrolyte, which was conducive to the rapid transfer of electrons between the (Ni0.5Co0.5)2P nanosheets and the PCNF substrate. The Tafel slopes were analyzed to explore the catalytic kinetics of HER, as shown in Fig. 5b. The Tafel slopes of (Ni0.5Co0.5)2P/PCNF, (Ni0.5Co0.5)2P/CNF, and (Ni0.5Co0.5)2P/PHCNF were 81, 108, and 113 mV dec−1, respectively. The smallest Tafel slope of (Ni0.5Co0.5)2P/PCNF indicates a faster HER catalytic kinetics, and the introduction of the pores into the CNF resulted in stable active sites for the electrode, enhanced conductivity, and a much shorter mass transport length. Additionally, (Ni0.5Co0.5)2P/PCNF exhibited much smaller charge transfer resistance (27.62 Ω) than the others listed in Table S1 (ESI†) according to Fig. 5c, revealing a fast electron transfer. The electrochemical active surface area (ECSA) could explain the roughness of the surface to a certain extent36,37 and was positively correlated with the value of the Cdl and evaluated by cyclic voltammetry (CV) plots at different scan rates (Fig. 5d and Fig. S10, ESI†) during the HER process. It was clear that (Ni0.5Co0.5)2P/PCNF had the largest Cdl (65.4 mF cm−2) which further confirmed the quick electron transfer ability and highly exposed active sites, which are important factors determining the electrocatalytic performance. In NiCoP, negatively charged P atoms act as proton acceptors, while positively charged metal atoms act as hydride acceptors, both of which are crucial active sites. Meanwhile, compared to transition metal oxides, TMPs have good conductivity and can more effectively accelerate charge transfer.
To further improve the HER performance of (Ni0.5Co0.5)2P/PCNF, Pt nanoparticles and (Ni0.5Co0.5)2P nanosheets were anchored on heteroatom-doped PCNF to prepare Pt-(Ni0.5Co0.5)2P/(X) CNF (X = B, S). The electrochemical properties were investigated in the same electrolyte. As seen in Fig. 6a, among all the obtained electrodes, Pt-(Ni0.5Co0.5)2P/SPCNF exhibited a much-reduced overpotential of 64 mV overpotential at a current density of 10 mA cm−2, well below those of Pt-(Ni0.5Co0.5)2P/PCNF (156 mV), Pt-(Ni0.5Co0.5)2P/BPCNF (323 mV), and Pt-(Ni0.5Co0.5)2P/BSPCNF (258 mV), which is almost on par with the performance of the Pt/C electrode (Fig. 6b). The ultra-high HER activity was attributed to the synergistic effect of the hybridized structure between Pt NPs and (Ni0.5Co0.5)2P. Doping with S could modulate the electronic structure of the carbon atom and enhance its catalytic kinetic process to reduce the overpotential. In addition, The Tafel slope (Fig. 6c) of Pt-(Ni0.5Co0.5)2P/SPCNF (74.9 mV dec−1) was the smallest among the as-prepared Pt-(Ni0.5Co0.5)2P/(X) CNF (X = B, S), indicating a favorable HER kinetics. The Nyquist plots (Fig. 6d) showed a reduced Rct value for the Pt-(Ni0.5Co0.5)2P/SPCNF (72.98 Ω), which was much lower than that of the others (Table S2, ESI†). Besides, the Cdl of the composites (Fig. 6f) could be evaluated by CV plots at different scan rates (Fig. S11, ESI†). The minimum charge transfer resistance for the EIS and the maximum electrochemical double layer capacitance of the ESCA demonstrate that Pt-(Ni0.5Co0.5)2P/SPCNF possesses the largest active surface area, with exposed active sites and the fast electron transfer ability. Sulfur doping of porous carbon fiber (S-PCNF) changes the electron cloud density of the C atom, resulting in defect sites against active sites.38,39 Except for the high electrocatalytic activity, the stability of Pt-(Ni0.5Co0.5)2P/SPCNF for HER was investigated by continuous CV cycles in 1M KOH at a scan rate of 50 mV s−1. After 2000 cycles, the overpotential (Fig. 6e) showed only small changes at a current density of 10 mA cm−2, indicating good stability of Pt-(Ni0.5Co0.5)2P/SPCNF in an alkaline electrolyte.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3nj04456d |
| This journal is © The Royal Society of Chemistry and the Centre National de la Recherche Scientifique 2024 |