Junchao Xiongab,
Xiaohong Chen
*a,
Yupan Zhanga,
Yue Luc,
Xundao Liuc,
Yafei Zheng
a,
Yongming Zhanga and
Jun Lin
b
aInstitute of Advanced Materials, North China Electric Power University, Beijing, 102206, China. E-mail: xhchen200905@ncepu.edu.cn
bSchool of New Energy, North China Electric Power University, Beijing, 102206, China
cSchool of Materials Science and Engineering, University of Jinan, Jinan, 250022, China
First published on 18th January 2022
The development of non-noble metal catalysts with high-performance, long stability and low-cost is of great importance for fuel cells, to promote the oxygen reduction reaction (ORR). Herein, Fe/Co/N–C/graphene composites were easily prepared by using Fe/ZIF-67 loaded on graphene oxide (GO). The Fe/Co/porous carbon nanoparticles were uniformly dispersed on graphene with high specific surface area and large porosity, which endow high nitrogen doping and many more active sites with better ORR performance than the commercial 20 wt% Pt/C. Therefore, Fe/Co/N–C/graphene composites exhibited excellent ORR activity in alkaline media, with higher initial potential (0.91 V) and four electron process. They also showed remarkable long-term catalytic stability with 96.5% current retention after 12000 s, and outstanding methanol resistance, compared with that of 20 wt% Pt/C catalysts. This work provides an effective strategy for the preparation of non-noble metal-based catalysts, which could have significant potential applications, such as in lithium–air batteries and water-splitting devices.
Although some non-noble metal supported nitrogen–carbon catalysts have higher initial potentials and half-wave potentials than that of commercial Pt/C catalysts, their durability still remains a great challenge. Recently, many efforts have been made to improve the durability of the electrochemical catalysts, such as increasing the surface area and enhancing the degree of graphitization.32–34 Heteroatom doped carbon materials derived from metal–organic frameworks (MOFs) have been considered as the ideal ORR catalyst materials, because of their adjustable and porous structure.35–42 Zeolitic imidazolate frameworks (ZIFs), one of the most promising precursor materials among the MOF family, possessed large surface area, high porosity and adjustable pore size.43–45 More importantly, ZIFs are rich in nitrogen and can offer active center metals to afford high activity for fuel cells.46–49 However, the calcination from ZIFs will destroy their ordered structure and porous morphology, leading to the poor ORR performance, which is attributed to the low graphitization, poor conductivity and electron migration ability of ZIFs materials. With NaCl as additives, porous Co/N co-doped catalysts were prepared by the calcination of ZIF-67, which showed excellent ORR performance.50 Co, Fe, Ni co-doped nitrogen-rich hollow carbon (CoFeNi/NC) derived from PVP/ZIF-8/ZIF-67 exhibited relatively good ORR catalytic activity. The addition of Fe and Ni can enhance the graphitization degree and the specific surface area of the CoFeNi/NC, to substantially enhance the ORR activity.51 To further enhance the ORR performance of ZIFs-based catalysts, it is urgent to prepare catalysts with high specific surface area and high electrical conductivity.
Generally, graphene oxide (GO) with large surface area, rich graphitic carbon and excellent electrical conductivity is widely used in fuel cell and other fields.52–56 Herein, we developed a simple and effective preparation method of Fe/Co/N–C/graphene composites, derived from Fe/ZIF-67 (2-methylimidazole cobalt/iron) loaded on GO. Interestingly, Fe/Co/N–C/graphene composites showed excellent ORR catalytic activity in the alkaline electrolyte. The initial potential and half-wave potential, limiting current density and electron transfer number (n) of Fe/Co/N–C/graphene composites were better than that of 20 wt% Pt/C catalysts. Moreover, Fe/Co/N–C/graphene composites also displayed excellent stability and methanol resistance in the alkaline media.
To observe the morphology of the prepared samples, scanning electron microscopy (SEM) of ZIF-67, ZIF-67/GO, Fe/ZIF-67, Co/N–C, Co/N–C/graphene and Fe/Co/N–C was characterized. Fig. 1a shows ZIF-67 has regular polyhedral shape and uniform size (about 1 μm), confirming the successful synthesis of ZIF-67 crystals. Fig. 1b shows the carbon skeleton of Co/N–C derived from ZIF-67 was collapsed and contracted, losing its original regular shape and structure. The surface of Co/N–C becomes rough and the size decreases, mainly due to the decomposition of imidazole and the cleavage of organic ligands during pyrolysis. After the addition of GO, ZIF-67 nanoparticles become larger and are unevenly dispersed on the surface (Fig. 1c). There are many microspheres in Co/N–C/graphene (Fig. 1d). Even though the introduction of GO can promote the formation of graphitic nitrogen, the mass transfer efficiency in the microspheres may not be high due to the lack of pores. Therefore, Fe/ZIF-67 presents regular polyhedral shape (Fig. 1e), due to the Fe addition. Moreover, the morphology of Fe/ZIF-67 with smooth surface and large size (Fig. 1f) could be retained during the pyrolysis process.
![]() | ||
Fig. 1 SEM images of (a) ZIF-67, (b) Co/N–C, (c) ZIF-67/GO, (d) Co/N–C/graphene, (e) Fe/ZIF-67 and (f) Fe/Co/N–C composites. |
Fig. 2a–c show SEM images of Fe/ZIF-67/GO under different magnification factors. Fe/ZIF-67/GO remains regular polyhedral structure with the addition of GO and Fe. Fe/ZIF-67 nanoparticles is uniformly dispersed on the GO surface, which can prevent the collapse of the carbon skeleton and the accumulation of GO during the pyrolysis process. Fe/Co/N–C nanoparticles with a size of about 30 nm are distributed on the graphene (Fig. 2d–f). To get more information of the surface area and porosity of the Fe/Co/N–C/graphene, the N2 adsorption and desorption isotherms of ZIF-67, Fe/ZIF-67/GO, Co/N–C and Fe/Co/N–C/graphene are shown in Fig. 2g and h. ZIF-67 and Fe/ZIF-67/GO exhibit large specific surface areas (293.5 and 573.1 m2 g−1), and abundant macropores and mesopores (2.5 and 4.9 nm) (Fig. 2h). The surface area and average pore diameter of Co/N–C/graphene is 78.4 m2 g−1 and 6.7 nm (Fig. S1†), while the specific surface areas and large pore size of Co/N–C and Fe/Co/N–C/graphene are (131.1 m2 g−1, 7.3 nm) and (150.4 m2 g−1 and 8.1 nm), respectively. The larger pores and smaller surface area of Fe/Co/N–C/graphene may be caused by the co-addition of Fe3+ and GO. The increase in the pore size of Fe/Co/N–C/graphene can ensure fass diffusion of oxygen, leading to the improvement of the catalytic activity of Fe/Co/N–C/graphene.
To get more information of Co/N–C and Fe/Co/N–C/graphene structure, the transmission electron microscopy (TEM) characterization of Co/N–C and Fe/Co/N–C/graphene was conducted. The Fe/Co/N–C nanoparticles of Fe/Co/N–C/graphene were uniformly dispersed on the graphene, with the well-distributed particle size (about 10–30 nm) (Fig. 3a). In comparison, the Co/N–C nanoparticles were agglomerated (Fig. S2†), without the addition of Fe and graphene. High resolution TEM (HRTEM) of Fe/Co/N–C/graphene composites shows that the lattice spacing is 0.191 nm and 0.202 nm, respectively, which corresponds to the crystal plane of metal Co (101) and Fe–Co (330). These results indicate the Co and Fe–Co alloy nanoparticles appear together in Fe/Co/N–C/graphene, which could offer more active sites for enhancing ORR performance. It is also clear from Fig. 3b that Fe/Co/N–C particles are uniformly dispersed on the surface of graphene, indicating that graphitic carbon in Fe/Co/N–C/graphene around metal ions was easily formed, which also enhances the catalytic activity of ORR. Furthermore, Fig. 3e shows a high-angle annular dark field scanning transmission electron microscope (HAADF-STEM) and corresponding element mapping image of Fe/Co/N–C/graphene, which shows the carbon and nitrogen dopants are uniformly distributed in the Fe/Co/N–C nanoparticles. Meanwhile, Co and Fe elements are well distributed and match with N region, indicating that Co–Nx and Fe–Nx active sites may be formed in these samples. The energy dispersion spectrometer (EDS) results of Fe/Co/N–C/graphene composites showed the weight content of C, N, Co and Fe (Fig. 3f) is 81.24 wt%, 2.51 wt%, 1.82 wt% and 4.39 wt%, respectively, which is consistent with the HAADF-STEM results.
The XRD spectra of Co/N–C, Co/N–C/graphene, Fe/Co/N–C and Fe/Co/N–C/graphene were further analyzed. The peaks of ZIF-67, ZIF-67/GO, Fe/ZIF-67 and Fe/ZIF-67/GO are similar (Fig. S3†), indicating that the addition of Fe3+ and GO has little influence on the crystal structure of ZIF-67. As shown in Fig. 3g, three diffraction peaks of Co/N–C, Co/N–C/graphene and Fe/Co/N–C composites were at 44.31°, 51.68° and 76.08°, respectively, which are consistent with the Co (111), Co (200) and Co (220) (PDF#150806) crystal plane, indicating the successful formation of Co crystals in these composites. The diffraction peaks at 35.45°, 43.84° and 45.00° were also observed in Fe/Co/N–C/graphene, which are well matched with Fe–N (400), Fe–Co (330) and Co (101) (PDF#510740) crystal plane, and also consistent with the TEM results. Furthermore, Raman spectra of Co/N–C, Co/N–C/graphene, Fe/Co/N–C and Fe/Co/N–C/graphene were performed to analyze their defect degree (Fig. 3h), in which two characteristic carbon peaks were shown, corresponding to D band peak of 1348 cm−1 and G band peak of 1599 cm−1, respectively. The intensity ratio of the two peaks (ID/IG) was used to evaluate the defect degree of the catalysts.57 The ID/IG of Fe/Co/N–C/graphene composites is 1.05, which is higher than that of Co/N–C (1.04), Co/N–C/graphene (1.00) and Fe/Co/N–C (1.01) composites, due to many more defect sites in the carbon skeleton produced by Fe dopants and graphene. This may provide more active ORR sites and have good mass transfer ability.
To probe the chemical element composition and chemical state, XPS tests of Co/N–C and Fe/Co/N–C/graphene were further performed. The C, N, O, Co and Fe elements of the Fe/Co/N–C/graphene composites are shown in Fig. 4a and Table 1. Graphitic-N and pyridinic-N play important roles in ORR performance,58 which is of great significance to the understanding of electrocatalysis. The high resolution N 1s (Fig. 4d) of Fe/Co/N–C/graphene can be divided into six types: pyridine-N (398.8 eV), graphitic-N (401.5 eV), pyrrolic-N (400.8 eV), Co–N (399.5 eV), Fe–N (399.6 eV) and oxygen-N (403.8 eV), and the corresponding atomic contents are 11.36, 27.32, 8.58, 25.44, 5.84 and 21.46% (Table 2), respectively. Compared with that of Co/N–C, the overall N content of Fe/Co/N–C/graphene increased, especially with the sharp increase of the graphitic-N and Co–N contents. These results suggested that the Fe/Co/N–C/graphene owns high content of graphitic-N, higher specific surface area, more Co–Nx and Fe–Nx active sites, and better mass transfer efficiency, which is attributed to the addition of Fe and GO.
![]() | ||
Fig. 4 (a) XPS survey scan of Co/N–C and Fe/Co/N–C/graphene; the XPS spectra of (b) N 1s, (c) Co 2p for Co/N–C and (d) N 1s, (e) Co 2p, (f) Fe 2p for Fe/Co/N–C/graphene. |
Samples | C 1s (%) | N 1s (%) | O 1s (%) | Co 2p (%) | Fe 2p (%) |
---|---|---|---|---|---|
Co/N–C | 93.04 | 1.36 | 4.87 | 0.73 | — |
Fe/Co/N–C/graphene | 89.42 | 2.02 | 6.41 | 1.3 | 0.85 |
Samples | Oxidized-N (%) | Graphitic-N (%) | Pyrrolic-N (%) | Pyridinic-N (%) | Co–N (%) | Fe–N (%) |
---|---|---|---|---|---|---|
Co/N–C | 34.78 | 10.75 | 8.07 | 32.96 | 13.44 | — |
Fe/Co/N–C/graphene | 21.46 | 27.32 | 8.58 | 11.36 | 25.44 | 5.84 |
The Co–Nx and Fe–Nx are one of the most effective active sites to improve the catalytic activity of ORR performance under alkaline conditions. As seen in Fig. 4e, two main peaks of the Co 2p spectra of Fe/Co/N–C/graphene were observed, corresponding to Co2p1/2 (797.2 eV) and Co2p3/2 (780.5 eV), respectively. Co2p3/2 can be divided into Co0 (780.0 eV), Co–O (781.2 eV), Co–Nx (782.9 eV) and satellite peak (787.0 eV), respectively. Co–O may be due to the oxidation of Co on the surface of GO, and Co–N confirms the existence of Co–Nx, which can increase the catalytic activity of ORR under alkaline conditions.59 The Fe 2p spectra (Fig. 4f) show Fe 2p3/2 (711.6 eV), Fe 2p1/2 (724.3 eV), satellite peak (716.1 eV) and Fe0 (719.5 eV), indicating that Fe not only acts as an additive to form uniform dispersion and many more pores of ZIF-67, but can form the active sites of Fe–Nx to enhance the ORR performance. In addition, Co0 in Co 2p and Fe0 in Fe 2p confirm the presence of Fe–Co alloy, which can also improve the catalytic activity of Fe/Co/N–C/graphene.
To evaluate the ORR performance of Co/N–C, Co/N–C/graphene, Fe/Co/N–C and Fe/Co/N–C/graphene, their CV measurements were carried out at a potential scan rate of 100 mV s−1 through a three-electrode system in O2-saturated 0.1 M KOH.60 As seen in Fig. 5a, the CV curves of Co/N–C, Co/N–C/graphene, Fe/Co/N–C and Fe/Co/N–C/graphene show large cathodic reduction peaks at 0.81 V, 0.84 V, 0.78 V and 0.87 V, respectively, indicating the Fe/Co/N–C/graphene composite has a larger oxygen reduction peak. The LSV curves of Co/N–C, Co/N–C/graphene, Fe/Co/N–C and Fe/Co/N–C/graphene composites were recorded in Fig. 4b. Fe/Co/N–C/graphene composites have excellent ORR electrocatalytic activity with the limiting current density of 6.78 mA cm−2, which is slightly higher than that of 20 wt% Pt/C (6.63 mA cm−2). It can be seen from Table 3 that Co/N–C/graphene has a corrected initial potential (Eonset) at 0.89 V and half-wave potential (E1/2) at 0.83 V, which is higher than that of Co/N–C (0.86 V, 0.81 V) and Fe/Co/N–C (0.85 V, 0.81 V). This is attributed to the enhanced electrical conductivity and increased activity sites with the addition GO. However, the change of Eonset and E1/2 is relatively small with the addition of Fe. Furthermore, with the co-addition of GO and Fe, the Eonset and E1/2 of Fe/Co/N–C/graphene are 0.91 V and 0.85 V, which were higher than that of 20 wt% Pt/C (0.91 V, 0.82 V), indicating that Fe/Co/N–C/graphene composites had a remarkable ORR activity. This is due to the enhanced electrical conductivity and more Co–Nx and Fe–Nx active sites with the coincorporation of Fe and GO. The limiting current density of the Co/N–C, Co/N–C/graphene, Fe/Co/N–C and Fe/Co/N–C/graphene (Fig. 5d–f, S4a and c†) increased with the increasing rotation rate from 400 to 2000 rpm, suggesting higher diffusion rate of O2 to improve ORR activity.
According to the Koutecky–Levich (K–L) diagram (Fig. 5d, e inset, S4b and d†), the average electron transfer number (n) of Fe/Co/N–C and Co/N–C/graphene composites at 0.2–0.6 V was calculated to be 3.13 and 3.80, respectively. Moreover, the n of Co/N–C and Fe/Co/N–C/graphene composites in the range of 0.2–0.6 V was 3.94 and 4.02, respectively, indicating that it was a favorable 4e− oxygen reduction pathway in the ORR process, which produces water instead of intermediate products such as H2O2 during the ORR process. Furthermore, the electrochemical activity comparison between Fe/Co/N–C/graphene and other previously reported catalysts is summarized in the Table 4, which shows Fe/Co/N–C/graphene has the better ORR performance. From the slope of the corresponding Tafel curve (Fig. 5f), the Tafel slope of Fe/Co/N–C/graphene is 70.25 mV dec−1, which was lower than that of Co/N–C (71.98 mV dec−1), Co/N–C/graphene (111 mV dec−1), Fe/Co/N–C (144 mV dec−1) and 20 wt% Pt/C (158 mV dec−1). These results further confirmed the excellent ORR activity of Fe/Co/N–C/graphene composites, due to the synergistic effect among the graphene, graphitic-N, Co–Nx and Fe–Nx activity sites.
Samples | Eonset (V vs. RHE) | E1/2 (V vs. RHE) | JL (mA cm−2) | n | Ref. |
---|---|---|---|---|---|
Fe/Co/N–C/graphene | 0.91 | 0.85 | 6.78 | 4.02 | This work |
ZIF-67-900 | 0.91 | 0.82 | 5.33 | 3.52 | 23 |
NGR | 0.87 | 0.74 | 5.63 | 3.40 | 30 |
CoNC-CNFs | 0.92 | 0.80 | 5.91 | 3.98 | 37 |
Zn–Co–ZIF/GO-920 | 0.91 | 0.81 | 6.23 | 3.97 | 45 |
CoNC–1NaCl-800 | 0.94 | 0.84 | 5.43 | 4.17 | 49 |
CNT-900 | 0.93 | 0.81 | 4.98 | 3.99 | 61 |
FeCo/Co2P@NPCF | 0.85 | 0.79 | 4.89 | 3.85 | 62 |
In addition, to further assess the mechanism of enhanced ORR activity on Fe/Co/N–C/graphene, we identified the electron transfer numbers and the peroxide (H2O2) yield using a rotating ring disk electrode (RRDE). As shown in Fig. 6a, the H2O2 yield is below 8% and the n value within the potential of 0.2–0.9 V is 3.84 during the ORR process, which is better than Co/N–C (Fig. S5†). This demonstrates a dominant four-electron ORR catalytic pathway. Therefore, the RRDE result for Fe/Co/N–C/graphene is in accordance with that of the RDE.
To gain further insight into the catalytic efficiencies of the Co/N–C, Co/N–C/graphene, Fe/Co/N–C and Fe/Co/N–C/graphene, the turnover frequencies (TOF) and Cdl of Co/N–C and Fe/Co/N–C/graphene were calculated. Compared to that of Co/N–C (19.25 mol O2 min−1 catalyst min−1), the TOF of Fe/Co/N–C/graphene catalyst displayed a higher value of 49.18 mol O2 min−1 catalyst min−1, indicating the increasing average intrinsic active sites in Fe/Co/N–C/graphene. Cdl was used to evaluate the largest electrochemical active surface area (ECSA) of the electrode, which can be measured via the CVs in non-faradic potential range at various scan rates. The half value of linear slope for ΔJ vs. scan rate plots represents the Cdl. Fig. 6b and Fig. S6† show the CV curves of Co/N–C, Co/N–C/graphene, Fe/Co/N–C and Fe/Co/N–C/graphene at different scanning rates, whose Cdls were obtained according to the corresponding calculation. As seen in the Fig. 6c, the calculated Cdl of Fe/Co/N–C/graphene electrode (45.46 mF cm−2) is higher than that of Fe/Co/N–C (16.34 mF cm−2), Co/N–C (43.69 mF cm−2) and Co/N–C/graphene (37.72 mF cm−2), which indicates the Fe/Co/N–C/graphene has the largest ECSA. Because the catalytic activity of the electrode material is dependent on the ECSA, Fe/Co/N–C/graphene shows the highest catalytic activity.
Apart from the electrocatalytic activity, the long-term stability of the catalysts is the key index for their application in fuel cells. Therefore, the catalytic durability of Co/N–C, Fe/Co/N–C/graphene and 20 wt% Pt/C composites was evaluated by measuring i–t chronoamperometric response at 0.62 V in O2-saturated 0.1 M KOH at 1600 rpm. As shown in Fig. 7a, after 12000 s, 96.5% of the initial current for Fe/Co/N–C/graphene was retained, compared with 91.2% for Co/N–C and 89.3% for 20 wt% Pt/C. The excellent stability of Fe/Co/N–C/graphene is attributed to the increased graphitic carbon of nanoporous carbon particles after the addition of GO. Moreover, methanol solution (3.0 wt%) was added to O2-saturated 0.1 M KOH solution at 200 s to test the methanol resistance of Co/N–C, Fe/Co/N–C/graphene and 20 wt% Pt/C (Fig. 7b). The current of 20 wt% Pt/C sharply decreased, resulting from the toxic effect of methanol on Pt, while the current of Co/N–C, and Fe/Co/N–C/graphene wasn't changed, demonstrating much better methanol tolerance than 20 wt% Pt/C. These results indicate that Fe/Co/N–C/graphene has better ORR performance, superior durability and excellent methanol resistance, which makes it a promising fuel cell catalyst material as the alternative for the commercial Pt/C catalyst.
As shown from the sketch of the catalytic mechanism in Fig. 8, Fe/Co/N–C/graphene composites exhibited better ORR electrocatalytic activity with the addition of Fe and graphene, which is attributed to the following factors: (1) with the addition of Fe, the porosity of ZIF-67 could be retained during the pyrolysis process. More Co–Nx active sites are provided and Fe–Nx active sites are generated for improving ORR performance; (2) with the addition of graphene, there are high specific surface area and much more active sites to enhance the catalytic activity. The high electrical conductivity of graphene could increase the mass transfer efficiency. These special features endow Fe/Co/N–C/graphene with excellent stability and high electrocatalytic activity.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1ra08817c |
This journal is © The Royal Society of Chemistry 2022 |