Yueyue Cao,
Lanfang Wang,
Moyan Chen and
Xiaohong Xu*
Key Laboratory of Magnetic Molecules and Magnetic Information Materials of Ministry of Education, School of Chemical and Material Science, Shanxi Normal University, Linfen, 041004, China. E-mail: xuxh@sxnu.edu.cn
First published on 7th June 2021
A tungsten-based electrocatalyst for hydrogen evolution reaction is vital for developing sustainable and clean energy sources. Herein, W2N/WC composite nanofibers were synthesized through electrospinning technology and simultaneous carbonization and N-doping at high temperature. The composite nanofiber has higher catalytic activity than any simple compound. It exhibits remarkable hydrogen evolution performance in acidic media with a low overpotential of −495 mV, at a current density of −50 mA cm−2. The excellent hydrogen evolution performance of the composite nanofiber could be attributed to the abundant active sites, strong light absorption and fast charge transfer. The method used in this work provides a new possibility for the fabrication of high-performance electrocatalysts rationally.
Among the earth-abundant and inexpensive catalysts, tungsten-based catalysts, such as carbides and nitrides, have gained considerable interest for HER because of their unique properties, such as Pt-like electronic structure, good electrical conductivity and chemical inertness in acidic and basic solutions.14–16 Especially, due to the narrow band gap of 2.2 eV, W2N was usually used as a potential photocatalyst for photoelectrochemical hydrogen production.17 Moreover, it has been theoretically and experimentally displayed that tungsten nitride/tungsten carbide (W2N/WC) heterostructure catalyst exhibits outstanding synergistic enhancement in HER activity, which is much better than their individual material.18–20 On account of this, a great deal of fabrication methods has been used to prepare the heterostructure, including solvothermal, solid-state synthesis and colloidal chemistry.21–23 Unfortunately, as a notably general technique to prepare nanofibers with more active sites, electrospinning is rarely used to prepare W2N/WC heterostructure nanofibers.
In this work, W2N/WC heterostructure nanofibers have been successfully synthesized by using electrospinning technology and simultaneously carbonization and N-doping at high temperature. This synthesized W2N/WC heterostructure nanofiber is displayed remarkable photoelectrochemical hydrogen production performance. The nanofiber architecture exposes more active sites for electrochemical HER. The light harvesting as well as the interface between W2N and WC facilitates charge transport and thus promotes HER kinetics. We believe that it is a versatile way to develop heterostructure materials with better conductivity and HER activity.
Fig. 2a–f shows SEM images of the as-spun precursor nanofibers and WO3 nanofibers annealed at different temperature (470–510 °C). It can be clearly observed that the precursor nanofibers have good continuity with a diameter of about 500 nm, and the surface of nanofiber is smooth. After annealed at high temperature, the surface of nanofiber begins to show some bumps and unevenness. With the increase of annealing temperature, there are more and more non-smooth scaly protrusions on the surface of the sample, which is consistent with the results of existing reports.24,25 Fig. 2g shows the XRD patterns of the as-spun precursor nanofibers and WO3 nanofibers treated with different annealing temperatures (470–510 °C). After high temperature treatment, the sample begins to show the characteristic peaks of WO3. The diffraction peak appearing at 20–25° corresponds to the composite peaks of WO3 (001), (020) and (200), the peak at 30–35° corresponds to the composite peak of WO3 (021), (201) and (220). The appearance of recombination peak may be due to the poor crystallinity of WO3 annealed at lower temperature. As the annealing temperature increases, the peaks at 20–25° and 30–35° begin to appear split peaks, and some new, weaker characteristic peaks appear. The peak at 28.7° corresponds to WO3 (111), the peak at 41.5° corresponds to WO3 (221). The positions of various peaks correspond to the standard XRD pattern of WO3 (PDF#20-1324).26 It can be seen that with the annealing temperature increases, the diffraction peaks become more and more obvious, which means the increased crystallinity of sample. In the subsequent high-temperature conversion treatment, the sample should not only have the typical diffraction peak of WO3, that is, good crystallinity, but also have good fiber continuity and cannot be broken. So we choose the nanofiber annealed at 490 °C undergoes subsequent high temperature carbonization and N-doping.
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Fig. 2 SEM images of the as-spun precursor nanofibers (a) and WO3 nanofibers annealed at 470 °C (b), 480 °C (c), 490 °C (d), 500 °C (e) and 510 °C (f). The corresponding XRD images (g). |
After carbonization and N-doping, the SEM images of nanofibers prepared at different conversion temperatures (600–1000 °C) are shown in Fig. 3a–f. It can be observed that the nanofibers still maintain a linear morphology without adhesion during the high-temperature conversion process. As the annealing temperature increases, the diameter of nanofibers tends to decrease. This may be because the crystallinity of nanofibers becomes better at high temperatures and nanofibers become denser.17,27 Fig. 3g shows the XRD patterns of nanofibers treated with different conversion temperatures. When the conversion temperature is 600 °C, the characteristic peak of W2N first appears. The characteristic peak at 37.7° can be well in line with the (111) plane of W2N. The characteristic peak at 43.8° can be attributed to (200) of W2N, which corresponds to W2N (PDF#25-1257).20 There is no WC characteristic peak at all, indicating that all nanofibers are nitrided to W2N. When the conversion temperature reaches 750 °C, the characteristic peak of WC begins to appear. The peak at 48.3° can match with WC (101), corresponding to WC (PDF#51-0939).18 This indicates that the W2N/WC heterostructure nanofiber was constructed. As the temperature increases, the content of WC gradually increases, and the content of W2N gradually decreases. When the conversion temperature reaches 1000 °C, the characteristic peaks of WC appear, corresponding to WC (001), WC (100), WC (101). There are almost no characteristic peaks of W2N, which means that the nanofibers annealed at 1000 °C are mainly WC. Therefore, by controlling the annealing temperature, we can adjust the degree of carbonization of WO3 nanofibers, and adjust the content of WC in the W2N/WC composite nanofibers to transform pure W2N into W2N/WC composites, eventually transformed into WC.
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Fig. 3 SEM images of the nanofibers after carbonization and N-doping at 600 °C (a), 700 °C (b), 750 °C (c), 800 °C (d), 900 °C (e) and 1000 °C (f). The corresponding XRD images (g). |
To investigate the effect of conversion temperatures on the catalytic performance, the catalytic properties of nanofibers toward HER were measured in 0.5 M H2SO4 solution. Fig. 4a displays the LSV curve of CFP, WO3, as well as carbonization and N-doping W2N/WC composite nanofibers. They are tested under dark conditions. The tested voltage range is 0 V to −0.9 V (V vs. Ag/AgCl). The speed is 10 mV s−1. It can be seen that as the conversion temperature increases, the onset overpotential decreases and then increases. The W2N/WC composite nanofibers treated at 750 °C have the smallest onset potential, the required overpotential is approximately −516 mV at −50 mA cm−2. This indicates that the W2N/WC composite nanofibers treated at 750 °C have the largest hydrogen evolution catalytic activity. Fig. 4b is the EIS diagram of each sample tested at −0.8 V. It can be seen that the W2N/WC composite nanofibers treated at 750 °C have the smallest arc radius, which means smaller resistance and fast interface charge transfer.1,28 Therefore, the W2N/WC composite nanofibers treated at 750 °C have a relatively small overpotential, which can correspond well to Fig. 4a.
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Fig. 4 (a) LSV curve and (b) EIS diagram of CFP, WO3, carbonization and N-doping W2N/WC composite nanofibers at different temperatures (600–1000 °C). |
In order to clearly elucidate the increasing catalytic activity of W2N/WC composite nanofibers treated at 750 °C, we tested the electrochemically active specific surface area (ECSA) of each sample. The CV curve with different scan rates (5, 10, 15, 20, 25, 30 mV s−1) was used to characterize the electrochemical capacitance behavior of the sample with the same apparent area in the faradaic zone. Fig. 5a–h shows the CV curves of different samples in 0.5 M H2SO4 solution. According to the following formula, the double-layer capacitance Cdl (mF) of different samples can be obtained:29
Cdl = I/n |
In order to further analyze the morphology and composition of W2N/WC composite nanofibers treated at 750 °C, we conducted transmission electron microscopy (TEM) and selected area electron diffraction. Fig. 6a is the TEM image of W2N/WC nanofiber. It can be seen that the nanofibers have uniform diameters and rough surfaces, showing good nanofibers morphology. Fig. 6b is a high-resolution transmission electron microscope image. It can be seen that the lattice spacing of 0.23 nm correspond to the (111) plane of W2N, and the lattice spacing of 0.18 nm corresponds to the (101) plane of WC. The diffraction rings in the selected area electron diffraction pattern are shown in Fig. 6c, which can corresponds to the (111), (200), (222) crystal planes of W2N and the (101), (110) crystal planes of WC, respectively.20 Fig. 6d–g is the element mapping diagram of W, C, and N. Obviously, the elements of W, C, and N are evenly distributed on the nanofibers. These results confirm that the nanofibers treated at 750 °C are W2N/WC composite nanofibers.
In order to identify the surface elements and valence state information of the W2N/WC composite nanofibers treated at 750 °C, X-ray photoelectron spectroscopy (XPS) are shown in Fig. 7. Fig. 7a is the XPS total spectrum. We can observe the presence of W, C, N, and O elements. Fig. 7b is a high-resolution W 4f spectrum. The two peaks at the lower binding energy of 32.2 and 34.4 eV are typical characteristic peaks of W–C.31,32 The peaks at 35.6 and 37.9 eV are attributed to the W–N bond.33 Fig. 7c is the spectrum of C 1s. The peak at 284.5 eV can be attributed to the existence of the W–C bond. The N 1s spectrum in Fig. 7d also proves the existence of the N–W bond. The fitting peaks at 398.8 and 401.6 eV can be attributed to the characteristics of the N–C bond, while the peak at 397.6 eV is attributed to the N–W bond.34 This further confirms the formation of W2N/WC composite nanofibers.
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Fig. 7 (a) W2N/WC nanofiber XPS total spectrum; (b) W 4f; (c) C 1s; (d) N 1s high-resolution XPS image. |
The photoelectrocatalytic HER performance of WO3, W2N (treated at 600 °C), W2N/WC (treated at 750 °C) and WC (treated at 1000 °C) was also investigated. Fig. 8a is the LSV curve of different samples under simulated sunlight. Compared with W2N and WC catalyst, the onset overpotential of W2N/WC composite catalyst is smaller. When a current density of −50 mA cm−2 is obtained, the W2N/WC composite catalyst only needs an overpotential of −495 mV, which is much lower than that for W2N catalyst (−549 mV), WC catalyst (−619 mV) and WO3 catalyst (−641 mV). This means that W2N/WC composite catalyst has the highest hydrogen evolution performance. Noteworthily, these values are lower than that for the corresponding catalysts under dark condition (as shown in Fig. 4a). Fig. 8b shows the photocurrent response (I–t) results of various catalysts. Compared with WO3, W2N and WC catalysts, W2N/WC composite catalysts have greater photocurrent response. The corresponding ultraviolet-visible absorption spectrum is shown in Fig. 8c. W2N/WC composite catalyst has a stronger light absorption than W2N and WC, and has a wider absorption spectrum than WO3, which means the maximize use of sunlight. Fig. 8d is an EIS image under simulated sunlight. W2N/WC catalyst also shows the smallest interface resistance, which means that the interface charge transfer rate is faster. Nevertheless, the larger ECSA, stronger light absorption and faster charge transfer in the W2N/WC composite nanofiber are largely responsible for such excellent hydrogen evolution performance.
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