Thiruparasakthi Balakrishnan,
Mohamed Anis,
S. Arun,
Mithin Kumar,
Sakthivel Arun kumar and
Sundar Mayavan*
CSIR-Central Electrochemical Research Institute, Karaikudi, India. E-mail: sundarmayavan@cecri.res.in
First published on 15th August 2016
A simple one-step procedure for the preparation of nanosheets of crystalline 2D boron carbon nitride containing cobalt oxide (Co3O4–BCN) involving glycine–nitrate combustion chemistry is reported. The as-prepared hybrid is a highly active catalyst for dye degradation, and for the water oxidation reaction as compared to pristine Co3O4. Co3O4–BCN shows enhanced catalytic activity for the oxygen evolution reaction (OER) in alkaline electrolyte. The onset potential towards the OER is 0.406 V (vs. Ag/AgCl) in 1 M KOH. A current density of 10 mA cm−2 has been achieved at an overpotential of 394 mV in 1 M KOH. The as-prepared hybrid exhibits highly-efficient degradation ability for methyl orange and methyl blue dyes under direct sunlight irradiation.
The XRD pattern of as-prepared Co3O4–BCN (Fig. 1a) exhibits a broad peak between 22 and 26° and at 42°, which is similar to (002) and (100) lattice planes of BCNs reported previously with h-BN structures.12 Interestingly, the XRD pattern of Co3O4–BCN does not show any peak originating from cobalt species in line with the previously reported cobalt-containing carbon nitride compounds.13 But XRD pattern of Co(NO3)2 thermally treated at 500 °C for two hours showed characteristic cobalt oxide peaks (Fig. 1a). This is an indication that the cobalt species is chemically coordinated to the BCN host.13 Fig. 1b shows FTIR spectra of the Co3O4 and Co3O4–BCN hybrid materials. The Co3O4 spectra showed two peaks at 576 cm−1 and 665 cm−1 for metal oxide (Co–O) stretching vibrations. Co3O4–BCN hybrid materials shows a large absorption band at 1380 cm−1 which is due to stretching mode of B–N in the hexagonal boron nitride. The band at 702.04 cm−1 is due to stretching of Co–O and is shifted to higher wavelength as compared to Co3O4 due to interaction between cobalt oxide between BCN host. Absorption bands due to C–N and cubic-BN are assigned to be at 1618 cm−1 and 1043 cm−1, respectively.14,15 Based on the above FTIR result it may be said that Co3O4–BCN hybrid structures are achieved. The Raman spectra of Co3O4–BCN (Fig. 1c) exhibited two peaks corresponding to the D band (at 1355 cm−1) and G band (at 1581 cm−1), along with a Co–O band at 743 cm−1.16 Hence, the Raman data indicates the presence of both BCN structures and cobalt oxide. In Fig. 2, the absorption properties of BCN–Co3O4 are compared with those of the pristine Co3O4. The as-prepared BCN–CO3O4 is characterized by a significantly improved absorption in the visible light range than the Co3O4.
Fig. 3 shows the XPS spectra of as-prepared hybrid. Survey spectra (Fig. 3a) indicate the presence of B, C, N, O and Co species. The high resolution C 1s spectra (Fig. 3b) show a major peak at 284.3 eV and a small shoulder at 285.7 eV corresponding to CC bonds, and C
N respectively.17 It also shows a tail in the higher binding energy region which indicates the presence of small amount of oxygen containing groups. High resolution B 1s spectra (Fig. 3c) of the as-prepared sample show a major peak at 190.9 eV, which indicates the presence of boron in the form of B–N.18 This suggests that the main bonding configuration for B in our films is similar to that of h-BN. The N 1s spectra (Fig. 3d) show a major peak with a binding energy of 398.2 eV which correspond to N in h-BN.19 Both the B 1s and the N 1s spectrum indicate that the main configuration for the B and N atoms is the B–N bond, implying that h-BN domains exist in the film. High resolution XPS spectrum of cobalt (Fig. 3e) showed doublet spectral lines at binding energies of 778.7 eV (Co 2p3/2) and 794.9 eV (Co 2p1/2) with energy separation of 15.6 eV, which indicates the presence of cobalt in divalent form.20 The smaller at around 800 eV correspond to satellite peaks, resulting from shake excitations.21 The high resolution O 1s spectrum (Fig. 3f) shows a peak at 530.1 eV, which correspond to the oxygen species from Co3O4.20
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Fig. 3 Survey (a) and high resolution spectra of carbon (b), boron (c), nitrogen (d), cobalt (e) and oxygen (f). |
The morphology of the as-prepared Co3O4–BCN was characterized by field emission scanning electron microscopy (FE-SEM). FE-SEM image (Fig. 4b) reveals porous layered morphology as compared to spherical shaped pristine Co3O4 particles (Fig. 4a). EDX spectra (Fig. S1†) confirm the presence of B, C, N, O, and Co species. The elemental mapping (Fig. S2†) indicates homogeneous distribution of B, C, N, Co, and O species. Sonication was used as a top–down method to exfoliate layered Co3O4–BCN sheets. Representative TEM images (Fig. 4c) show that the exfoliated CoO–BCN sheet morphology resembles that of highly crumbled and randomly aggregated graphene-like sheets. SAED pattern (Fig. 4d) indicates the crystalline nature of the as-prepared Co3O4 hybrid. The Co3O4 samples were also investigated by nitrogen adsorption and desorption measurement at 77 K. As shown in Fig. 3d, the nitrogen adsorption–desorption curves demonstrate a Type IV isotherm and the specific surface areas of Co3O4 and BCN–Co3O4 have been 24.17 and 107.19 m2 g−1, respectively. The BET result is consistent with the SEM observations discussed above, showing porous structure with relatively high interfacial area. The structural feature gives implications of the applications in catalysis.
The electrochemical performances of the prepared materials were analysed using cyclic voltammetry (CV). Fig. 5a shows the CV curves of Co3O4 and BCN–Co3O4 electrodes at a scan rate of 50 mV s−1 between 0 and +0.6 V (vs. SCE) in 1 M KOH aqueous electrolyte. A typical single redox peak for cobalt oxide has been observed in the CV curves.16 On the other hand, BCN containing cobalt oxide exhibit a larger CV area than that of pristine Co3O4, indicating a higher specific capacitance compared with the Co3O4 without BCN. Fig. 5b shows the cyclic voltammograms as a function of scan rate for BCN–Co3O4. With the increase of the scan rate, the current response increases. A quasi-linear relationship is observed between the redox peak current and the scan rate, indicating a diffusion-controlled process and dominant surface redox reactions.
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Fig. 5 (a) Cyclic voltammetry curves of Co3O4 and BCN–Co3O4; (b) CV of BCN–Co3O4 at different scan rates; (c) LSV curves of Co3O4 and BCN–Co3O4 for OER. |
The water oxidation catalytic activities of the as-synthesized nanocomposites were first investigated in alkaline solution (1 M KOH) in a standard three-electrode setup. Linear sweep voltammetry (LSV) curves of BCN–Co3O4 catalyst is shown in Fig. 5c. BCN–Co3O4 catalyst exhibits significantly higher anodic current and lower onset potential than that of the Co3O4 catalyst, in 1 M KOH solutions (Fig. 5c). In 1 M KOH solution, BCN–Co3O4 catalyst shows a sharp onset potential at 0.406 V (vs. Ag/AgCl), and achieves the current density of 10 mA cm−2 at the overpotential of 397 mV, which is much better than that of the Co3O4, Co3O4/SWNTs (593 mV)4 and mesoporous Co3O4 catalysts (525 mV)8 in the same alkaline solution. This shows that BCN can be used as support for Co3O4. Through our work we have shown that BCN can be used as a potential material for supporting Co3O4 towards OER. The excellent electrochemical performance of BCN–Co3O4 catalyst suggests its promising application towards OER both in alkaline solution. A series of controlled experiments, shown in Fig. 5, have demonstrated that the obtained BCN–Co3O4 catalyst displayed better OER activity than those of pure Co3O4 in 1 M KOH conditions. The strong interaction of Co3O4 nanoparticles with BCN nanosheets and the unique architecture have strong effect on the catalytic property of the composite. This further illustrates that the strong chemical coupling and good interaction between the Co3O4 and BCN can significantly improve the electron transport and reaction kinetics during the OER. In order to further investigate the high performance of BCN–Co3O4, the effective surface areas were estimated, which was determined by electrochemical capacitance measurements from static cyclic voltammetry. The capacitance for BCN–Co3O4 is much higher than Co3O4 (Fig. 5a). Therefore, the high performance could be also associated with the high electro active surface area. In addition, the unique and intimate contact between the BCN and Co3O4 contributes to the superior catalytic activity. The photocatalytic activity of BCN–Co3O4 catalyst was tested by examining the degradation of MB and MO dye solution as a function of time under direct sunlight irradiation. Fig. 6a shows the photocatalytic activities of the sample under direct sunlight irradiation. A blank experiment was performed with MO dye in water under the same conditions, but without any catalyst, to exclude the possible photolysis of the dye under direct sunlight irradiation. No or very low MO degradation was observed in the absence of catalyst. Only 19% of the MO was degraded by pure Co3O4 (control) in 2 h (data not shown here). Using BCN–Co3O4 sheets leads to 89.13% photo degradation of MO in about 4 min (Fig. 6a). The MO and MB dye exhibits a characteristic absorption peak at 473 nm and 664.22,23 Fig. 6b shows that the degradation of MO dye (the quenching of the MO absorbance peak by 90.33%) and a decrease in colour compared with the original solution was clearly observed. These results demonstrate that the BCN–Co3O4 showed excellent photocatalytic activity compared with pristine Co3O4. The BCN–Co3O4 also degrades MB in 4 minutes with 92.1% efficiency under same experimental condition. Thus, the as-prepared catalyst degrades both the methylene blue and methyl orange dye effectively with above 90% efficiency in less than 5 minutes without any accelerators, which is much better than that of the Co3O4-g-C3N4 (complete degradation occurs in 3 hour),24 Co3O4 nanoparticles (4 hour in presence of H2O2 accelerator)25 and Co3O4/GO (6 minutes in presence of peroxymonosulfate accelerator).26 The rate of the reaction is also determined by the calculating rate constant value for MO and MB degradation (Fig. S3†). Further to understand the effect of visible range, a control experiment was done under sunlight with UV filter. With UV filter the degradation efficiency decreases only about 3–4% (Fig. S4†). The stability and reusability of the Co3O4–BCN catalyst was studied in repeated degradation reaction of MO and MB. The catalyst was reused (three times) after each reaction by simple filtration and washing with water. The reused catalyst displayed consistent reactivity with less than 3% decrease in efficiency (Fig. S5a†). The stability of catalyst after dye degradation is analysed by comparing the FTIR spectra of samples before and after dye degradation. It is observed from the Fig. S5† that there are no changes in bonding characteristics of the spectra. This confirms there is no dislocation of bonding or modification of bonding upon recycling which proves the material is highly stable.
In summary, for the first time we have shown that BCN can be used as a support material to encapsulate Co3O4 via thermal treatment involving glycine, copper nitrate and B2O3. The obtained hybrid shows enhanced catalytic activity for OER in alkaline electrolyte as compared to pristine Co3O4. The onset potential towards the OER is 0.405 V (vs. Ag/AgCl) in 1 M KOH. The current density of 10 mA cm−2. The as-prepared hybrid also exhibits high-efficient degradation ability for methyl orange (MO) and methyl blue (MB) dyes under direct sunlight irradiation as compared to pristine Co3O4.
Footnote |
† Electronic supplementary information (ESI) available: Experimental details, reusability of the Co3O4–BCN for dye degradation. See DOI: 10.1039/c6ra16058a |
This journal is © The Royal Society of Chemistry 2016 |