Kun
Wang
,
Jiawei
Guo
and
Hui
Zhang
*
State Key Laboratory of Chemical Resource Engineering, Beijing University of Chemical Technology, Beijing, 100029, China. E-mail: zhanghui@buct.edu.cn; huizhang67@gst21.com
First published on 29th July 2022
Herein, we have prepared a series of highly efficient bifunctional electrocatalytic composites, NixFe1-LDH/rGO/NF (x = 3, 2, 1), with vertically staggered NiFe-LDH nanosheets grown on nickel foam uniformly modified with reduced graphene oxide through a simple green hydrothermal method. The as-obtained nanosheet-array-like composites exhibit excellent performance for the oxygen evolution reaction (OER) and hydrogen evolution reaction (HER). In particular, Ni2Fe1-LDH/rGO/NF requires 228 and 109 mV for the OER and HER in 1 M KOH at 10 mA cm−2, respectively. Moreover, when it is directly used as both cathode and anode at the same time for overall water splitting, it only requires 1.62 V to achieve 10 mA cm−2. The as-prepared Ni2Fe1-LDH/rGO/NF composite shows excellent electrocatalytic performance, which is ascribed to the unique array-like nanosheet framework with exposed paths, the synergy between Ni2Fe1-LDH and rGO, and the vertically staggered growth of Ni2Fe1-LDH on the rGO/NF substrate improving the stability. This strategy can also be applied to create composites of other metal compositions with a nanosheet-array-like structure as efficient electrocatalysts for the development of efficient clean renewable energy.
Layered double hydroxides (abbreviated as LDH) are layered inorganic materials that have the following structural characteristics: two-dimensional ordered layered structure, uniform dispersion of the main laminate elements, adjustable chemical composition of the main laminate, adjustable guest types and quantities and a diversity of structures, for which these compounds have attracted wide attention.21,22 Various LDH materials with different compositions, such as NiFe LDH23,24 and CoFe LDH,25 have been extensively studied in recent years. However, their active sites are less available due to their poor conductivity.26 Carbon nanofibers,27 carbon nanotubes28 and graphene29 have great potential in electrocatalysis owing to their large specific surface areas, satisfactory stability and conductivity. The combination of LDH and graphene is of important research significance, as it can significantly compensate for the low conductivity of LDH and further enhance its electrochemical catalytic activity. For instance, Xia et al. synthesized RGO-Ni–Fe LDH using a simple solvothermal method, which only requires 250 mV to achieve 10 mA cm−2.30 However, powder catalysts need to be fixed to conductive substrates with the help of adhesives, and this will reduce the contact area between the electrolyte and catalyst and the conductivity of the catalyst, which will inevitably reduce the electrocatalytic performance.31 In addition, the catalyst will peel off the substrate because of its relatively weak binding force, especially under strong deflation conditions,32 and the stability of the electrode will also be reduced. Nickel foam (NF) has been widely used as a base material.33 Lu et al. reported a material using NF as the substrate to grow NiFe-LDH in situ, and the sample only required 280 mV at 30 mA cm−2 in the OER.34 Li et al. prepared NiFe-LDH/RGO/NF through an ordinary electrodeposition strategy, and the overpotential for achieving 10 mA cm−2 during the OER process was only 150 mV. The excellent performance may have been due to the synergy of its large electrochemical active surface area and conductive RGO interface.35 The catalyst synthesized by the electrodeposition method has a low yield and high requirements in terms of conditions, which is not suitable for large-scale commercial applications. Therefore, a need for improvement in preparation methods, catalytic performance, stability and applications remains. Thus, it is still a major issue in this field to obtain a bifunctional electrocatalyst that is suitable for commercial applications and shows outstanding overall water splitting performance using simpler methods and shorter time consumption.
In the present work, we develop an uncomplicated way to prepare array-like NiFe-LDH composites with vertically staggered nanosheets on rGO-modified NF using a hydrothermal method. The as-prepared composites, especially Ni2Fe1-LDH/rGO/NF, have a highly uniform nanosheet-array-like morphology decorated with tiny flowers, endowing the composite with strong synergy between Ni2Fe1-LDH and rGO/NF and structural stability. The vertically staggered growth of Ni2Fe1-LDH on the rGO/NF substrate is also favourable to the stability. The structure, composition, and macroscopic and microstructure morphology of all electrocatalysts were systematically characterized, and their electrochemical properties were also studied. Ni2Fe1-LDH/rGO/NF exhibits the highest electrochemical properties and excellent stability over at least 24 h, and its overall water splitting performance is greatly improved compared with those of recently reported electrocatalysts.
Scheme 1 Schematic of the synthesis strategy of NixFe1-LDH/rGO/NF (x = 3, 2, 1) composites with nanosheet-array-like morphology. |
The XRD patterns of the NixFe1-LDH/rGO/NF (x = 3, 2, 1) composites are shown in Fig. 1A. All the composites present strong and sharp diffraction peaks at 2θ values of 44.5°, 51.8° and 76.4° indexed to the (111), (200) and (220) crystal planes of Ni foam (JCPDS 04-0850),37 and small but detectable peaks corresponding to the (003) (11°) and (110) (59°) planes of the LDH phase (Ni0.75Fe0.25(CO3)0.125(OH)2·0.38H2O JCPDS 40-0215)38 due to the masking of the extremely strong diffractions of NF. The patterns of scraped powder samples from the NixFe1-LDH/rGO/NF (x = 3, 2, 1) composites shown in Fig. 1B clearly display sharp and symmetrical characteristic diffractions at 11.4°, 22.9°, 34.4°, 45.9°, 59.9°, 61.3° and 65.1° indexed to (003), (006), (012), (015), (018), (110) and (113) planes, respectively, and no other peaks of miscellaneous phases, implying that hexagonal NiFe-LDH was successfully synthesized in the obtained composites. The (003) peak with a basal spacing of 0.78 nm suggests the presence of interlayer CO32− anions, and the sharp (110) and (113) lines imply the ordered atomic dispersion state of metal cations on the LDH layers. It is also noted that the obvious peak at ∼11° (0.85 nm) corresponding to the (001) plane of GO36,39,40 disappears in the composites, implying the transformation of GO into rGO; this phenomenon is attributed to the reduction in the alkaline synthetic environment, and the change is beneficial for the improvement of the conductivity of the material. These findings clearly demonstrate the homogeneous combination of a well-crystallized LDH phase and rGO/NF. Table S1 (ESI†) shows the XRD structure parameters of the powder samples of the composites. The D110 data of the NixFe1-LDH/rGO/NF (x = 3, 2, 1) composites calculated according to the Scherrer formula are 21.63, 24.75 and 29.74 nm, respectively. From this, along with the strength and symmetry of the diffractions, it can be inferred that Ni2Fe1-LDH/rGO/NF possesses higher crystallinity and relatively smaller crystalline size.
The Raman spectra presented in Fig. 1C strongly verify the existence of rGO in the composites. The two obvious Raman bands at 1350 and 1592 cm−1 represent the D-band associated with the defect sites at the edge of graphene and the G-band related to the in-plane vibration of sp2 carbon atoms for carbon materials, respectively. The strength ratio of the D-band to the G-band (ID/IG) is generally applied to measure the degree of disorder of carbon and the average size of the sp2 region,41 and thus, the graphitization degree of the composites. The higher ID/IG value of Ni2Fe1-LDH/rGO/NF (1.26) compared with that of GO indicates that the graphitization degree of the composites is higher than that of the original GO (0.95), which was attributed to the unrepaired defect sites generated during the reduction of GO to rGO. The highest ID/IG value of Ni2Fe1-LDH/rGO/NF indicates that it has the most abundant defect sites, which can provide more catalytically active sites. In addition, the two weak bands near 596 and 662 cm−1 are attributed to Ni–O and Fe–O symmetric stretching vibrations, respectively.
The constructions of the composites were analyzed using SEM to further observe the morphologies. The SEM and (HR)TEM images of the NixFe1-LDH/rGO/NF (x = 3, 2, 1) composites, along with the EDS and elemental mappings, are shown in Fig. 2, and the SEM images of NF, the substrate rGO/NF and Ni2Fe1-LDH/NF are shown in Fig. S1 and S2 (ESI†). The bare Ni foam showed a smoother surface, which consisted of some interconnected pores, which is favourable for providing abundant electron channels and large contact area between the electrolyte and the electrode material. The rGO/NF results show that after modification with rGO, the small holes disappeared and an rGO tier was present on the surface of the NF, with obvious rGO sheet layer wrinkles on the surface. The composites NixFe1-LDH/rGO/NF (x = 3, 2, 1) (Fig. 2(A–C)) clearly present an array-like morphology with a large number of vertically staggered LDH nanosheets grown on the substrate.
Fig. 2 SEM images of NixFe1-LDH/rGO/NF (x = 3, 2, 1: A, B, C), and TEM (B1), HRTEM (B2, inset: FFT), EDS and elemental mapping (B3) of Ni2Fe1-LDH/rGO/NF. |
In detail, the Ni3Fe1-LDH/rGO/NF composite with small LDH nanosheets of ∼195 × 25.6 nm shows poor uniformity with obviously agglomerated particles. With the decrease of the Ni/Fe molar ratio, the size and thickness of the LDH nanosheets gradually increased, in line with the XRD data. The Ni1Fe1-LDH/rGO/NF composite shows enlarged and thickened LDH nanosheets (∼742 × 76.7 nm) that are intimately stacked together. The Ni2Fe1-LDH/rGO/NF composite exhibits a clear vertically staggered nanosheet array morphology decorated with a small amount of tiny, loosely aggregated flowers on hexagonal LDH nanosheets with moderate size and thickness (∼626 × 37.5 nm) and abundant open spaces. Compared with the non-rGO modified composite Ni2Fe1-LDH/NF (∼1.6 × 0.1 μm), the size of the LDH nanosheets in Ni2Fe1-LDH/rGO/NF is also obviously smaller (Fig. S2, ESI†).
The TEM image of Ni2Fe1-LDH/rGO/NF (Fig. 2B1) further reveals the nanosheet array morphology decorated with small flowers on the surface of the rGO. The HRTEM result in Fig. 2B2 shows lattice fringes of 0.231 and 0.197 nm, which were indexed to the (015) and (018) planes of Ni2Fe1-LDH nanosheets. Due to the influence of the Ni foam, the Ni:Fe atomic ratio of Ni2Fe1-LDH/rGO/NF obtained using EDS was 3.56:1. We used ICP to obtain a more accurate element ratio, and the obtained proportion was 1.95:1, which is close to that of the feedstocks. The elemental mappings (Fig. 2B3) indicate the uniform distribution of the elements Ni, Fe, C and O on the Ni2Fe1-LDH/rGO/NF composite. The relatively sparse dots in the image of the element C are consistent with the vertically staggered coverage of LDH nanosheets.
Based on the above microstructural features of the composites, it can be envisioned that their mechanical stability and durability may be greatly enhanced by the present network with abundant open space and high openness. Thus, the as-prepared novel composite electrodes can increase the effective contact area with the electrolyte, thereby promoting the rapid dispersion of electrochemical active substances and effective electron transfer, which is favorable for water splitting.
XPS characterization was used to study the electrocatalyst to further explore the possible chemical valence states and surface composition of the composites. The full XPS spectra of the NixFe1-LDH/rGO/NF (x = 3, 2, 1) composites (Fig. S3, ESI†) clearly affirm the presence of nickel, iron, carbon and oxygen. The XPS narrow spectra of the samples are presented in Fig. 3. Ni 2p XPS shows peaks at ∼874.7 and ∼857.0 eV, which were attributed to Ni 2p1/2 and Ni 2p3/2,42 respectively, and the corresponding satellite peaks at ∼880.9 and 862.8 eV, implying the existence of Ni2+ in all the samples. It is noted that the BE of Ni 2p3/2 of Ni2Fe1-LDH/NF is 856.10 eV, ∼0.3 eV lower than that of pure Ni2Fe1-LDH (856.40 eV), showing an increase in the electron density of the Ni2+ core level after the introduction of NF. The BE values of Ni 2p3/2 of the three composites NixFe1-LDH/rGO/NF (x = 3, 2, 1) are 856.00, 855.70 and 855.91 eV, respectively, which are 0.4, 0.7 and 0.49 eV lower than that of Ni2Fe1-LDH, respectively, demonstrating the obviously improved proportion of Ni2+, and Ni2Fe1-LDH/rGO/NF has the greatest upshift. The protruding peaks at ∼726.4 and ∼713.6 eV seen in the Fe 2p XPS are attributed to Fe 2p1/2 and Fe 2p3/2,43 respectively, affirming the existence of Fe3+. The BE value of Fe 2p3/2 of Ni2Fe1-LDH/NF is 713.00 eV, which is 0.19 eV higher than that for Ni2Fe1-LDH (712.81 eV), demonstrating that the combination of LDH and NF clearly reduces the electron density of Fe3+. In addition, the BE values of Fe 2p3/2 of the three composites NixFe1-LDH/rGO/NF (x = 3, 2, 1) are 713.30, 713.60, and 713.40 eV, respectively, which are 0.49, 0.79, and 0.59 eV higher than that of Ni2Fe1-LDH, respectively, indicating a decrease in the electron density of Fe3+, with Ni2Fe1-LDH/rGO/NF having the largest decrease. Based on these results, an obvious Ni–Fe synergistic effect exists in the composites due to electron transfer from Fe cores to Ni cores. The strongest synergy of Ni2Fe1-LDH/rGO/NF indicates the best activity.
Fig. 3 Ni 2p, Fe 2p, C 1s and O 1s XPS spectra of NixFe1-LDH/rGO/NF (x = 3, 2, 1: a, b, c) composites and Ni2Fe1-LDH/NF, Ni2Fe1-LDH, rGO/NF and GO. |
The C 1s XPS spectra of all the samples can be deconvoluted into four peaks assigned to CC, CO, C–O and O–CO at BE values (eV) of 284.6, 286.4, 285.4 and 288.9, respectively.44 The proportion of CC functional groups of rGO/NF (27.32%) is significantly higher than that of the initial GO (23.11%), indicating the partial reduction of the GO. The CC contents of Ni3Fe1-LDH/rGO/NF (30.97%), Ni2Fe1-LDH/rGO/NF (37.89%) and Ni1Fe1-LDH/rGO/NF (33.73%) are all higher than the initial GO (23.11%), consistent with the above Raman results, suggesting that more GO was converted to rGO in the synthesis environment, thus improving the conductivity. The CC content of Ni2Fe1-LDH/rGO/NF had the largest increase, indicating the strongest interaction between Ni2Fe1-LDH and the substrate.
The O 1s XPS spectra of all the samples can be deconvoluted into three peaks (Fig. 3) ascribed to the hydroxyl group (OI) in H2O (∼532.8 eV), the M–OH group (∼531.8 eV) (OII) and the M–O (M = Ni, Fe) group (OIII) on the LDH layer (∼531.0 eV).45 The BE value of the M–OH group of Ni2Fe1-LDH/NF is 531.11 eV, which is 0.02 eV higher than that of 531.09 eV of Ni2Fe1-LDH, indicating the reduced electron density of the M–OH group of LDH grown on NF. For the NixFe1-LDH/rGO/NF (x = 3, 2, 1) composites, the BE values of the M–OH group are 531.19, 531.40 and 531.20 eV, which are 0.1, 0.31 and 0.11 eV higher than that of Ni2Fe1-LDH (531.09 eV), respectively, in which Ni2Fe1-LDH/rGO/NF exhibits the biggest upshift, implying that its M–OH groups have the lowest electron density. In addition, the M–O contents of Ni3Fe1-LDH/rGO/NF (30.86%), Ni2Fe1-LDH/rGO/NF (35.83%), Ni1Fe1-LDH/rGO/NF (33.73%) and Ni2Fe1-LDH/NF (23.07%) are all higher than that of Ni2Fe1-LDH (22.47%).
All the above results tentatively reveal the existence of interaction between the electrons of the composites, and further demonstrate the synergistic impact of Ni–Fe, which has a positive effect on adjusting the electronic environment of the Ni and Fe species, and indicate there is likely to be an improvement in the electrocatalytic activity. In addition, the electrical conductivity could be improved due to the change from GO to rGO, thereby increasing the electrical conductivity and further improving the electrocatalytic performance of the composites.
The OER performances of all the composites and control samples were tested in 1 M KOH. All the polarization curves acquired were corrected with 90% iR compensation.46 The results showed that Ni2Fe1-LDH/rGO/NF possesses the most prominent OER behavior, requiring only 228 mV at 10 mA cm−2, and its performance is clearly better than those of Ni3Fe1-LDH/rGO/NF (256 mV), Ni1Fe1-LDH/rGO/NF (244 mV), Ni2Fe1-LDH/NF (283 mV), Ni2Fe1-LDH/rGO (323 mV), Ni2Fe1-LDH (371 mV), the substrate rGO/NF (390 mV), pure NF (455 mV) and RuO2 (350 mV) (Fig. 4A, C, D and F). As shown in Fig. 4B and E, the Tafel slope (mV dec−1) of Ni2Fe1-LDH/rGO/NF is only 37.9, which is clearly smaller than those of Ni3Fe1-LDH/rGO/NF (55.3), Ni1Fe1-LDH/rGO/NF (47.3), Ni2Fe1-LDH/NF (77.2), rGO/NF (139.7), NF (179.1) and RuO2 (180), giving further confirmation of its superior OER performance. The specific steps for excellent electrochemical performance can be summarized as follows:47
OH− + * ↔ OH* + e− | (1) |
OH− + OH* ↔ O* + H2O + e− | (2) |
O* + OH− ↔ OOH* + e− | (3) |
OOH* + OH− ↔ O2 + H2O + e− + * | (4) |
As shown in Fig. 4H, there is almost no decay in the overpotential of Ni2Fe1-LDH/rGO/NF for the OER after the tests, indicating its comparative superior stability and robustness. The inset curves in Fig. 4H show that the LSV curve is close to the original curve, and that there is only a slight rise in the overpotential after the test. This slight change may be attributed to the slightly reduced specific surface area, subtle aggregation and mutual adhesion of the nanosheets, which are not conducive to mass transfer, resulting in the reduction in the performance. The detectably reduced size and thickness of the LDH nanosheets (Fig. S4, ESI†) is likely to be related to the gas continuously released from the electrocatalyst and partial etching in strong alkaline solution, leading to the shedding of the catalyst, and thus a reduction in the weight of the active material.
The HER performances of all the electrocatalysts were further examined. Moreover, the electrocatalytic properties of the commercially available benchmark 20% Pt/C were measured under identical testing conditions. Surprisingly, as displayed in Fig. 5A, C, D and F, the overpotential of Ni2Fe1-LDH/rGO/NF is only 109 mV at 10 mA cm−2, which is inferior to that of 20% Pt/C (20 mV), but extremely improved compared to those of Ni3Fe1-LDH/rGO/NF (131 mV), Ni1Fe1-LDH/rGO/NF (117 mV), Ni2Fe1-LDH/NF (151 mV), Ni2Fe1-LDH/rGO (159 mV), Ni2Fe1-LDH (162 mV), the substrate rGO/NF (170 mV) and pure NF (192 mV), implying the outstanding HER activity of Ni2Fe1-LDH/rGO/NF in alkaline solution. The Tafel slope (mV dec−1) of Ni2Fe1-LDH/rGO/NF (121.1) is lower than those of Ni3Fe1-LDH/rGO/NF (143.4), Ni1Fe1-LDH/rGO/NF (130.6), Ni2Fe1-LDH/NF (152.2), the substrate rGO/NF (171.1) and pure NF (182.8) (Fig. 5B and E), implying its excellent HER activity. The mechanism for HER can be summarized as the Volmer (eqn (5))–Heyrovsky (eqn (6)) mechanism given below in alkaline solution:48
H2O (l) + e− + * ↔ OH− (aq) + H* | (5) |
H* + e− + H2O (l) ↔ H2(g) + OH− (aq) + * | (6) |
Fig. 5H reveals that the overpotential exhibits almost no decay after the stability measurement of Ni2Fe1-LDH/rGO/NF for the HER, maintaining stable electrocatalytic activity in alkaline solution. Subsequently, we compared the LSV curves and SEM images of Ni2Fe1-LDH/rGO/NF before and after the stability measurements. It can be seen from the inset curves that the LSV curve after the test is similar to the original one and that there is no obvious decline in current density. It can be seen from the SEM images that although there is slight agglomeration, the nanosheet array morphology is still relatively complete (Fig. S5, ESI†), so the electrocatalytic performance is not significantly reduced. The LDH loading amount was obtained using thermogravimetric analysis (TGA, Fig. S9, ESI†), and the calculated data for the loading of LDH on the rGO/NF of NixFe1-LDH/rGO/NF (x = 3, 2, 1) composites and control sample Ni2Fe1-LDH/NF are 6.21, 5.19, 5.86 and 4.14 mg cm−2, respectively. The above findings can help us to understand the excellent HER performance of Ni2Fe1-LDH/rGO/NF with good long-term stability.
We further analyzed the samples of Ni2Fe1-LDH/rGO/NF after the stability measurements using XPS to study the changes in the chemical valence states (Fig. S8, ESI†). For the OER, the two prominent peaks near 854.8 and 873.6 eV were attributed to the 2p3/2 and 2p1/2 of Ni2+, and the prominent peaks near 856.8 and 877.2 eV were attributed to the 2p3/2 and 2p1/2 of Ni3+, indicating that the Ni2+ on the surface was partially oxidized to Ni3+ during the OER. The Ni2+/Ni3+ ratio is 5.42 and 0.35 at 10 and 100 mA cm−2, respectively, indicating that Ni2+ will be more oxidized to Ni3+ due to the violent release of oxygen bubbles at high current densities. In the Fe 2p XPS, no significant changes occurred. In the C 1s XPS, the ratios of oxygen-containing groups were 64.93% and 86.55% at 10 and 100 mA cm−2, respectively, increasing by 2.82% and 24.44% compared to before, indicating that the higher the current density, the greater the amount of carbon corroded and the greater the proportion of oxygen-containing groups. Although the change had no obvious effect on the performance of the composite, because more oxygen-containing groups can decrease the stability of the structure, there will probably be a certain impact on the durability of the catalysts. After the OER stability test at 10 mA cm−2, the ratios of OII and OIII changed by −4.72% and 1.15%, respectively, and the ratios of OII and OIII changed by −1.31% and −5.06% at 100 mA cm−2, respectively, implying that M–OOH (M = Ni, Fe) was formed on the surface of the composite (Table S6, ESI†). For the HER, none of the valence states of the four elements changed significantly, indicating the excellent stability of Ni2Fe1-LDH/rGO/NF for the HER.49
The electrochemical surface area (ECSA) is determined using cyclic voltammetry. The double-layer capacitance (Cdl, mF cm−2) of Ni2Fe1-LDH/rGO/NF was 81.5, which is better than those of Ni3Fe1-LDH/rGO/NF (47.4) and Ni1Fe1-LDH/rGO/NF (71.6) (Fig. S6, ESI†), and is nearly two, four and six times higher than those of Ni2Fe1-LDH/NF (41.5), the substrate rGO/NF (17.8) and pure NF (13.2) (Fig. S7, ESI†), respectively. It is well known that a high Cdl value represents an increase in ECSA, indicating the highest intrinsic activity of Ni2Fe1-LDH/rGO/NF. We further calculated the ECSA to confirm the excellent performance of the electrocatalyst. The ECSA values of the composites were obtained using the following equation: ECSA = Cdl/Cs, where Cs (0.040 mF cm−2) is the specific capacitance in alkaline electrolyte, and the ECSA is directly proportional to Cdl. The ECSA of Ni2Fe1-LDH/rGO/NF obtained using the equation is 2037.5, which is greater than those of Ni3Fe1-LDH/rGO/NF (1185) and Ni1Fe1-LDH/rGO/NF (1790), suggesting better electrocatalytic performance. In addition, the TOF values of Ni2Fe1-LDH/rGO/NF are 0.153 and 0.077 s−1 for the OER and HER at an overpotential of 300 mV, respectively, which are obviously higher than those of Ni3Fe1-LDH/rGO/NF (0.102 and 0.033 s−1, respectively), Ni1Fe1-LDH/rGO/NF (0.128 and 0.056 s−1, respectively) and Ni2Fe1-LDH/NF (0.088 and 0.021 s−1, respectively), indicating the high intrinsic activity of Ni2Fe1-LDH/rGO/NF. All the above results further justify the excellent electrochemical properties of Ni2Fe1-LDH/rGO/NF.
Given that Ni2Fe1-LDH/rGO/NF can effectively be used for the OER and HER, a two-electrode alkaline electrolytic cell with Ni2Fe1-LDH/rGO/NF as both the anode and cathode was constructed to investigate the overall water splitting performance. As shown in Fig. 6A, the formed two-electrode alkaline electrolytic cell needs only 1.62 and 2.06 V to achieve 10 and 100 mA cm−2, respectively. Compared with other reports, the activity of Ni2Fe1-LDH/rGO/NF is better than or at least equal to that of other non-precious transition metal materials for overall water splitting (Fig. 6D and Table S7, ESI†). Moreover, the chronoamperometry measurements of Ni2Fe1-LDH/rGO/NF at 10 and 100 mA cm−2 over 24 h showed excellent long-term stability (Fig. 6B). Comparing the LSV curves before and after the test (Fig. 6C), there are only slight overpotential losses of 0.01 and 0.11 V for achieving 10 and 100 mA cm−2 compared with the initial ones, respectively, further proving the excellent stability toward overall water splitting and the favorable corrosion resistance to the alkaline electrolyte, which are consistent with its superior performance for the OER and HER.
To further demonstrate the excellent catalytic performance of Ni2Fe1-LDH/rGO/NF, we measured the stability of the control sample Ni2Fe1-LDH/NF. It can be seen from Fig. S10 (ESI†) that Ni2Fe1-LDH/NF exhibits excellent stability at low current density, but its stability is significantly reduced at high current density. This can be attributed to the lack of the anchor chain effect provided by rGO, reducing the mechanical stability of the catalyst. In addition, the performance reduction of Ni2Fe1-LDH/NF is larger than that of Ni2Fe1-LDH/rGO/NF after the stability tests. The overpotential for the OER of Ni2Fe1-LDH/NF at 10 and 100 mA−2 decreased by 21 and 63 mV, respectively, and it decreased by 55 and 93 mV for the HER, and decreased by 0.06 and 0.17 V for overall water splitting. These findings can be attributed to the greatly reduced electrical conductivity and the elevated reaction energy barrier of the catalyst without the contribution of rGO, thus reducing the catalytic performance. In addition, other powder catalysts need to be fixed on the substrate with the help of a binder, so the active sites will be partially covered, and the electrical conductivity and bonding strength will be greatly reduced. Thus, it can be inferred that its stability is far inferior to that of the sample grown directly on NF. Based on the above results, the reasons for the optimal catalytic performance and stability of Ni2Fe1-LDH/rGO/NF can be summarized.
The superior electrocatalytic performance of Ni2Fe1-LDH/rGO/NF may benefit from the following aspects (Scheme 2): (1) the unique nanosheet array morphology with open channels providing a large number of active sites, higher surface area, a highly open pore structure, more electron transport paths and beneficial contact area for the electrolyte and electrode. (2) Strong synergistic interaction between Ni2Fe1-LDH and rGO/NF, with the effective combination of the two parts greatly improving the dispersibility and avoiding the stacking of Ni2Fe1-LDH nanosheets. Additionally, the synergy between the Ni and Fe cores can effectively improve the reaction kinetics and electrical conductivity, which in turn leads to the efficient performance of Ni2Fe1-LDH/rGO/NF. (3) The vertically staggered growth of Ni2Fe1-LDH on the rGO/NF substrate could also improve the stability of the composite and increase the rate of bubble detachment, thus further improving the kinetics of both the OER and HER and the efficiency and stability of the subsequent reactions. All the above advantages make Ni2Fe1-LDH/rGO/NF an excellent catalyst with outstanding electrocatalytic activity and long-term stability.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2ma00370h |
This journal is © The Royal Society of Chemistry 2022 |