Yanling Wu1, Yanmin Wang1, Zuoxu Xiao2, Miantuo Li1, Yongling Ding1, Mei-Li Qi1,3. 1. School of Transportation and Civil Engineering, Shandong Jiaotong University Ji'nan 250357 China beauty0507@163.com. 2. College of Science, China University of Petroleum (East China) Qingdao 266580 China. 3. Shandong Branden Medical Devices Co., Ltd Qihe 251100 China.
With the development of highly efficient oxygen reduction reaction (ORR) electrocatalysts, rechargeable metal–air batteries and regenerative fuel cells have become more widely used because the cathodic ORR is a rate-limiting process.[1,2] In general, platinum-based catalysts are considered the most active catalysts used for the ORR. They can support the 4-electron pathway even at relatively low overpotentials. However, problems such as anode crossover, high cost, severe intermediate poisoning, and lack of stability under electrochemical conditions are inevitable.[3]Recently, numerous research efforts have been made to find substitutes for Pt-based catalysts, leading to the development of novel ORR catalysts at a low cost. The substituting materials that have been reported involve transition-metal chemical compounds,[4,5] N-coordinated metals on the matrices of carbon,[6,7] carbon materials with element doping,[8,9] and even conductive polymers.[10] Among transition-metal oxide-based systems, Co3O4-based electrocatalysts with diverse nanostructures and sizes, such as mesoporous Co3O4,[11] Co3O4 porous sheets,[12] mesoporous Co3O4 nanowires,[13] and Co3O4 nanorods,[14] have gained considerable interest owing to their enhanced electrocatalytic capability, simple preparation procedure, low cost and environmentally friendly characteristics. However, poor electrical conductivity seriously hinders their further application. To date, the most effective way to solve the above problems has been to introduce carbon-based materials as supports, among which porous carbon nanowire arrays,[15] graphene,[16] and carbon nanotubes[17] are the most commonly used. N-doped carbon materials can significantly improve the stability and conductivity of Co3O4-based catalysts.[18] However, the catalysts of Co3O4/C materials tend to peel off substrate surfaces during continuous cycling, exhibiting poor stability. The underlying reason is that the Co3O4/C composites are mainly obtained by directly loading nanoparticles on the surface of carbon.[19,20] As a new precursor, the zeolite imidazolate framework (ZIF-67) has aroused great attention due to its high specific surface area, abundant pores and structural diversity.[21,22] Moreover, during the pyrolysis process, some of the N in the ZIF, which acts as a precursor, can enter the sp2 lattice of the graphite carbon crystal. Therefore, the electronic structure inside the carbon matrix will be changed, and active chemisorption sites will be created. N, as a heteroatom, is able to produce good synergistic effects by coordinating itself with free metal and functional elements.[23,24]In this work, we developed a simple route to synthesize Co/Co3O4@N-doped active carbon nanostructures (denoted as Co/Co3O4@NC) derived from the pyrolysis of a zeolite imidazolate framework (ZIF-67) and the economical, abundant and renewable biomass of poplar flowers. The resulting Co/Co3O4@NC catalyst, containing active sites from Co/Co3O4 and N-doped carbon, displays excellent ORR activity in 0.1 M KOH (Eonset = 0.94 V, E1/2 = 0.85 V, as well as a small Tafel slope of 90 mV dec−1), which, via a 4-electron pathway, has long-term durability and resistance to methanol poisoning. This absorption-reaction route offers a new approach for synthesizing ZIF materials on conductive substrates.
Materials and methods
Chemicals and characterization methods
Detailed information on the chemical reagents, characterization methods and electrochemical measurements is listed in the ESI.†
Preparation process of electrocatalysts
In a typical synthesis, the poplar flower (denoted as PL) was first cleaned and dried. Then, 1.0 g of poplar flower powder and 0.05 g of the ZIF-67 precursor were mixed in 20 mL of methanol and stirred for 24 h. The ZIF-67 precursor was synthesized in accordance with a previous reference.[25] The product was dried at 80 °C for 12 h, and after being cooled, the above mixture was uniformly ground. Carbonization was carried out in an inert atmosphere at 10 °C min−1 and kept at 800 °C for 3 h. After being cooled, cleaned and dried, the final target sample (named Co/Co3O4@NC) was obtained. For comparison purposes, PL-based porous graphite carbon materials (denoted as PL-bio-C) and Co-based N-doped carbon materials derived from the pyrolysis of ZIF-67 (named Co@NC) were prepared under the same conditions, as shown in Fig. 1.
Fig. 1
Schematic diagram showing the synthesis of the Co/Co3O4@NC catalytic material.
Results and discussion
Morphological and structural characterization
The morphological and structural details of the obtained electrocatalysts were tested by field-emission scanning electron microscopy (FE-SEM), transmission electron microscopy (TEM) and high-resolution TEM (HR-TEM). Fig. 2 shows the FE-SEM images of PL-bio-C, Co@NC, and Co/Co3O4@NC. First, the FE-SEM images show the grooved lamellar structure of the PL-bio-C material (Fig. 2a). The ZIF-67 precursor displays a cubic structure with relatively rough edges (Fig. S1, ESI†). After pyrolysis, the structure of the ZIF-67 precursor remains in Co@NC, but the size of the cubic nanostructure shrinks from 500 to 200 nm (Fig. 2b). As verified by comparison of Fig. 2a and b, the added particles from the ZIF-67 precursor are successfully loaded on the nanoparticles originating from the biomass materials of the poplar flower powder, and the dispersion of these nanoparticles is improved, as shown in Fig. 2c.
Fig. 2
Representative FE-SEM images of (a) PL-bio-C, (b) Co@NC, and (c) Co/Co3O4@NC.
The morphology of Co@NC and Co/Co3O4@NC was further examined with TEM. The TEM images of the Co@NC (Fig. S2†) display many clustered cube structures of approximately 200 nm, similar to the SEM images. After doping, some small inorganic dots (3 to 5 nm in diameter) were surrounded by a graphite carbon layer (Fig. 3a), suggesting that the active inorganic species were embedded successfully in the carbon material. As shown in Fig. 3b and c, the active species are dispersed on the surface of Co/Co3O4@NC. The following d-spacings, 0.34, 0.18, and 0.24 nm, are assigned to the (002) plane of graphite carbon, (200) plane of Co, and (311) plane of Co3O4, respectively.[26] The elemental mapping images (Fig. S3, ESI†) further indicate that Co, C, N, and O are distributed homogeneously on the Co/Co3O4@NC sample.
Fig. 3
(a) TEM image of the individual layer of Co/Co3O4@NC (inset shows the particle size distribution of Co/Co3O4@NC). Lattice fringe images of (b) graphitic carbon and (c) Co and Co3O4 taken from the rectangular region, as obtained from the high-resolution TEM of Co/Co3O4@NC.
The crystal structures of the as-prepared samples, PL-bio-C, Co@NC, and Co/Co3O4@NC, were evaluated by powder X-ray diffraction (PXRD) (Fig. 4a). The prepared samples of PL-bio-C and Co/Co3O4@NC reveal relatively broad (002) diffraction peaks at approximately 26° and observable characteristic (101) diffraction at ∼43°, indicating fairly disordered but chiefly sp2-hybridized graphitic structures.[27] Relatively sharp peaks from metallic Co (JCPDS no. 15-0806) can be observed except for a weak carbon peak at approximately 26° in the prepared Co@NC sample. Meanwhile, additional diffraction peaks can be well indexed to metallic Co (JCPDS no. 15-0806) and cubic phase Co3O4 (JCPDS no. 42-1467) detected in the PXRD pattern of Co/Co3O4@NC, suggesting the coexistence of Co and Co3O4 composites on the graphitic matrix of carbon,[28] which is in good accordance with the HR-TEM result mentioned above and the Raman results. The Raman spectra of undoped PL-bio-C and doped Co/Co3O4@NC (Fig. 4b) display two peaks appearing at approximately 1330 and 1590 cm−1, further disclosing the existence of the GC phase in all these PL-bio-C-based materials.[29] In the present case, the low ID/IG ratio of graphitic carbon in Co/Co3O4@NC (1.003) compared to that in pure PL-bio-C material (1.065) indicates a relatively high graphitization degree of Co/Co3O4@NC, which should be expected to decrease the barrier to charge transport.[30,31] To further study the surface area of doped and undoped PL-bio-C materials, nitrogen adsorption–desorption isotherms were obtained (Fig. S4 and Table S1, ESI†). The results show that since Co and Co3O4 particles are deposited on PL-bio-C, the surface area of Co/Co3O4@NC (30.38 m2 g−1) decreases quickly from that of PL-bio-C (201.43 m2 g−1, Table S4†). The pore width of Co/Co3O4@NC increases slightly compared with that of PL-bio-C, revealing that the Co and Co3O4 particles are uniformly deposited on the PL-bio-C surface instead of blocking the connected channel of PL-bio-C.[32]
Fig. 4
(a) PXRD patterns of PL-bio-C, Co@NC, and Co/Co3O4@NC and (b) Raman spectra of PL-bio-C and Co/Co3O4@NC.
X-ray photoelectron spectroscopy (XPS) tests were adopted to examine the surface composition as well as the chemical valence state of Co/Co3O4@NC. The corresponding results are shown in Fig. 5. Distinctive peaks of C, N, O, and Co in the survey spectrum provide the following elemental contents: C (80.61%), N (1.43%), O (17.08%) and Co (0.89%) (Fig. S5†). Furthermore, based on the inductively coupled plasma optical emission spectrometry (ICP-OES) results, the Co content of Co/Co3O4@NC in aqua regia solution (10 mL, 0.0151 g) is 0.7563%. In addition, the comparison of PL-bio-C, Co@NC, and Co/Co3O4@NC survey diagrams found that N was self-doped in the PL-bio-C materials (Fig. S5†). The high-resolution XPS spectrum for C 1s (Fig. 5a) can be divided into 4 peaks centered at 284.5, 284.8, 285.5 and 288.8 eV, which correspond to sp2-C, sp3-C, C–N and CO, respectively. Moreover, the high proportion of sp2-carbon (CC at 284.5 eV) further reveals that carbon is in graphitic form, helping to enhance the electron conductivity of carbon materials and improve ORR activity.[33] The fitted N 1s spectra for Co/Co3O4@NC centered at 398.2, 398.9, 400.5, and 401.7 eV in Fig. 5b can be assigned to pyridinic, Co–Nx, pyrrolic, and graphitic nitrogen, respectively. The formation of the Co–N bond is possibly due to the pyrrolic N and pyridinic N affording more negative charges and diffuse orbitals, which are easily used as metal coordination sites to form Co–Nx sites. The robust Co–Nx bonds in the Co/Co3O4@NC electrocatalysts advantageously prevent the migration and agglomeration of nanoparticles.[34] In addition, pyridinic N, graphitic N, and Co–Nx sites could provide active sites for the ORR, which are advantageous for improving the catalytic ORR activity.[35,36] Furthermore, by comparing the XPS spectrum of N 1 s for PL-bio-C, Co@NC and Co/Co3O4@NC, it was found that there was a high proportion of pyrrolic N in PL-bio-C and a high proportion of Co–Nx in Co@NC. The proportion of pyrrolic N and Co–Nx decreased after the addition of composite materials, which may have a certain influence on the ORR, as shown in Fig. S6.† The XPS spectrum of Co 2p (Fig. 5c) displays 2 core-level signal peaks located at approximately 781.3 and 797.1 eV, which are in agreement with Co 2p3/2 and Co 2p1/2, respectively. In addition, the ∼15.8 eV energy difference between the Co 2p3/2 and Co 2p1/2 peaks (named spin–orbit splitting) corresponds well to Co3O4.[37] The two core-level signal peaks can be segmented into seven branch peaks, representative of Co0 (779.9 eV), Co3+ (780.5 eV), Co2+ (781.8 and 797.3 eV), Co–Nx (783.7 eV), and 2 shakeup satellites (786.6 and 803.6 eV). Thus, the XPS result confirms the coexistence of Co3O4 and Co in the catalyst. Compared with Co/Co3O4@NC, in addition to the presence of the signal peaks of Co0 and Co–Nx from the XPS spectrum of Co 2p in the Co@NC (Fig. S7†), there are also Co–O peaks, which are due to the partial oxidation of the Co atomic surface by air.[38] The O 1s region of Co/Co3O4@NC in Fig. 5d can be deconvoluted into three different contributions at 531.4 (O1), 532.5 (O2) and 533.7 eV (O3). The sharp peak at 531.4 eV is attributed to the lattice oxygen (O2−) of Co3O4. The peaks at 532.5 and 533.7 eV are caused by oxygen-containing functional groups on the carbon surface.[39]
Fig. 5
High-resolution XPS curves of the (a) C 1s, (b) N 1s, (c) Co 2p, and (d) O 1s core levels for Co/Co3O4@NC.
Electrochemical properties
First, the electrocatalytic ORR performances of the doped (Co/Co3O4@NC), undoped (PL-bio-C) and Co@NC catalysts were successively examined by cyclic voltammetry (CV) in O2-saturated and N2-saturated 0.1 M KOH at 50 mV s−1 (Fig. 6a and Table S2, ESI†). Compared with the CV of PL-bio-C and Co@NC, the resulting Co/Co3O4@NC exhibited enhanced catalytic ORR activity, as evidenced by the shift of the peak potential to a more positive value, further confirming the effectiveness of the material synergy in enhancing the catalytic activity for the ORR.[40]
Fig. 6
(a) CV curves of PL-bio-C, Co@NC, and Co/Co3O4@NC in 0.1 M KOH at 50 mV s−1 (O2-saturated with solid lines and N2-saturated with dotted lines). (b) LSV curves of the as-obtained carbon catalysts and commercial 20 wt% Pt/C catalyst in O2-saturated 0.1 M KOH electrolyte (sweep rate: 10 mV s−1 and rotation speed: 1600 rpm). (c) LSV curves of Co/Co3O4@NC at multiple rotation speeds. (inset: K–L plots of Co/Co3O4@NC at multiple potentials). (d) Tafel plots of PL-bio-C, Co@NC, Co/Co3O4@NC, and 20% Pt/C obtained via the LSV data.
The ORR activities of the doped and undoped materials were further explored by linear sweep voltammetry (LSV) polarization curves (Fig. 6b). As a comparison, the ORR performance of Co/Co3O4@NC is much better than that of undoped PL-bio-C and Co@NC (Fig. 6b, S8, S9 and Table S2, ESI†). The order of ORR activities is PL-bio-C (Eonset = 0.81 V, E1/2 = 0.63 V, JL = −3.30 mA cm−2) < Co@NC (Eonset = 0.87 V, E1/2 = 0.68 V, JL = −3.86 mA cm−2) < Co/Co3O4@NC (Eonset = 0.94 V, E1/2 = 0.85 V, JL = −4.78 mA cm−2), indicating that the properties of the catalysts can be successfully improved by further treating the PL-bio-C materials, although the Brunauer–Emmett–Teller (BET) surface area of Co/Co3O4@NC is lower than that of PL-bio-C (Table S1, ESI†). In accordance with the CV study, the LSV curves reveal that Co/Co3O4@NC displays a high onset potential (Eonset) of 0.94 V and a high half-wave potential (E1/2) of 0.85 V. Though the limiting current density of 4.78 mA cm−2 for Co/Co3O4@NC is much lower than that of Pt/C, Co/Co3O4@NC exhibits better ORR performance than most of the electrocatalysts reported in the literature (Table S3†).To further reveal the advantages of Co/Co3O4@NC, LSV curves were obtained at various rotation speeds (400 to 2025 rpm), and the results are shown in Fig. 6c. The current density increases with increasing rotation speed. The Koutecky–Levich (K–L) plots illustrate that the electron transfer number (3.82) for Co/Co3O4@NC (inset of Fig. 6c) is higher than those for Co@NC (3.37) and PL-bio-C (2.69). This value is close to the value (4.0) observed with Pt/C (Fig. 6c, S8, S9, and Table S2†), implying that Co/Co3O4@NC follows the four-electron oxygen reduction path for the ORR.[41]Fig. 6d shows that the Tafel slope of the doped Co/Co3O4@NC (90 mV dec−1) is the smallest in comparison with that of Co@NC (216 mV dec−1), PL-bio-C (251 mV dec−1) and Pt/C (97 mV dec−1), indicating the fast electron transfer rate of the Co/Co3O4@NC catalyst.In an attempt to understand the much improved ORR activity on Co/Co3O4@NC, the double layer capacitance (Cdl) in the faradaic silent region provided an indication of the electrochemical active surface area (ECSA). The CV curves recorded in nitrogen purged 0.1 M KOH aqueous solution in the potential range from 0.0.5 to 0.15 V (Fig. S10a–c†). The evaluated Cdl values for Co/Co3O4@NC, Co@NC and PL-bio-C were 3.62, 1.39 and 2.28 mF cm−2 (Fig. S10d†), respectively, which indicated the presence of large amounts of electrochemical active centers in these materials; hence, Co/Co3O4@NC had better activity for the ORR in 0.1 M alkaline solution.[42]In practice, long-term durability is an important criterion for ORR catalysts with high efficiency. Here, a chronoamperometric response was obtained to measure the stability of Co/Co3O4@NC and Pt/C in O2-saturated 0.1 M KOH. The constant voltage and rotation rate were set at 0.8 V and 1600 rpm, respectively. Co/Co3O4@NC shows 75% retention of the initial current density over 10 000 s of continuous operation, while the Pt/C catalyst undergoes activity loss with only approximately 60% retention (Fig. S11a, ESI†). Consequently, the abundant nitrogen species in Co/Co3O4@NC may provide stable anchoring sites for the Co and Co3O4 active components, thus improving the dispersibility and stability of the active components on this carbon carrier.[39,43,44] Moreover, the methanol crossover experiment shows that the current density has no obvious interference on Co/Co3O4@NC when methanol is added to the electrolyte. In contrast, the Pt/C catalyst displays a sharp decrease in the current as a result of methanol oxidation (Fig. S11b, ESI†). Moreover, the chemical compositions and morphology of Co/Co3O4@NC after ORR long-term stability measurements were also investigated. The XRD patterns of Co/Co3O4@NC show diffraction peaks similar to the original peaks, proving that the chemical components of Co/Co3O4@NC were not transformed after the durability measurement and thus demonstrated excellent electrochemical stability (Fig. S12†). In the XPS spectrum of Co 2p, the ratios of Co 2p3/2 and Co 2p1/2 peaks respectively located at approximately 781.3 and 797.1 eV for Co/Co3O4@NC decreased from the initial ratio of 1.07/1 to 1.02/1. Otherwise, the initial sharp peak of Co/Co3O4@NC for O 1s at 531.7 eV moves toward a higher energy region (532.5 eV) after the ORR durability test, and a new peak at approximately 532.5 eV likely belongs to chemisorbed oxygen, which confirms the formation of Co(iii)OOH on the surface of Co/Co3O4@NC (Fig. S13†).[45] In addition, after the stability test, samples of the Co/Co3O4@NC catalyst were collected, and SEM data indicated that its morphological structure could still be maintained (as shown in Fig. S14†). These results indicate that Co/Co3O4@NC possesses higher ORR catalytic stability and better methanol resistance than the Pt/C catalyst. Furthermore, the reported Co/Co-based oxide electrocatalysts and their catalytic performances for the ORR are summarized in Table S3.† We can infer from Table S3† that the ORR electrocatalytic properties of Co/Co3O4@NC are no less than those of other Co/Co-based oxide-based electrocatalysts, demonstrating its superior catalytic activity.
Conclusions
In summary, we developed a low-cost and highly stable Co/Co3O4@NC catalyst for the ORR; Co–Co3O4 provided the active sites, earth-abundant poplar flowers were the carbon source and a zeolite imidazolate framework (ZIF-67) was the precursor. The doped atoms played significant roles in improving the ORR activity of the prepared electrocatalysts. This catalyst exhibited outstanding catalytic activities in 0.1 M KOH (Eonset = 0.94 V, E1/2 = 0.85 V, and a small Tafel slope of 90 mV dec−1), which, via a 4-electron pathway, had excellent stability and methanol resistance and was better than those of most currently reported cobalt-based catalysts. The unique Co–Co3O4 nanoparticles as well as N-containing functional groups in the Co/Co3O4@NC catalyst could provide abundant active sites to improve the interfacial electron transfer in the ORR system, thus enhancing the catalytic activity for the ORR. This work offers a cost-effective and scalable pathway to optimize the ORR performance of ZIF-derived electrocatalysts and an intriguing strategy to use sustainable and abundant biomass resources to design nonprecious carbon electrocatalysts.
Author contributions
Writing—original draft and writing—review & editing, Y.-l. W.; investigation, L.-m. T.; data curation, Y.-l. D.; supervision, Z.-x. X.; funding acquisition, Y.-m. W.; resources, M.-l. Q. All authors have read and agreed to the published version of the manuscript.
Authors: Hae-Kyung Jeong; Yun Pyo Lee; Rob J W E Lahaye; Min-Ho Park; Kay Hyeok An; Ick Jun Kim; Cheol-Woong Yang; Chong Yun Park; Rodney S Ruoff; Young Hee Lee Journal: J Am Chem Soc Date: 2008-01-08 Impact factor: 15.419