Abstract
In this present work, we synthesized a yolk-shell shaped CuCo2S4 by a simple anion exchange method. The morphological and structural properties of the as-synthesized sample were characterized using X-ray diffraction (XRD), UV-vis diffuse reflectance spectra (UV-vis DRS), scanning electron microscopy (SEM), and transmission electron microscopy (TEM). The SEM and TEM results confirmed that the uniform yolk-shell structure was formed during the solvothermal process. The band gap was about 1.41 eV, which have been confirmed by UV–vis DRS analysis. The photocatalytic property was evaluated by the photocatalytic degradation of methylene blue (MB) dye as a target pollutant under the visible-light irradiation. The experimental results confirmed the potential application of yolk-shell shape CuCo2S4 in visible-light photocatalytic applications.
Keywords: yolk-shell, structural, electron microscopy, semiconductors, photocatalyst
1. Introduction
Owing to their unique structural properties, as well as outstanding electrical properties, hollow nanostructures with tunable shape and size have gained huge research interest in the field of supercapacitors, catalysis, and biosensors [1]. The hollow architectures have relatively less density, high porosity, fast electron transfer, and higher surface area than the bulk materials. Up to date, various hollow structured metal oxides and sulfides have been successfully synthesized using soft and hard-template techniques [2]. For example, Y. Chen et al. fabricated Co3O4 hollow microspheres using Polyvinylpyrrolidone (PVP) as a template [3]. This synthesized hollow Co3O4 exhibits superior lithium storage capacity than the bulk Co3O4. S.E. Moosavifard et al. synthesized CuCo2O4 hollow spheres using a simple soft template route, which exhibits superior electrochemical than the bulk CuCo2O4 [4]. However, little attention has been paid by the research community to investigate the structural property of hollow metal sulfides [5]. In the past few decades, ternary metal sulfides have attracted great attention in the field of energy storage devices and photocatalysts due to their outstanding electrical properties. Among them, copper-cobalt sulfides (CuCo2S4) have been recognized as a promising material for pollutants degradation and water splitting, since they offer superior stability than other metal sulfides. CuCo2S4 is considered to be an environmentally benign material compared to CdS and In2S3 due to its low cost, less toxicity, and availability in nature [6]. In the past few decades, various morphologies of CuCo2S4, such as flowers, particles, and clusters have been successfully prepared using various approaches. In this work, we report a solvothermal route to synthesize a novel yolk-shell shaped CuCo2S4 using the sulfidation of Cu-Co glycerate precursor with thiourea. The prepared CuCo2S4 yolk-shell exhibited superior photocatalytic activity towards the degradation of MB dye under the visible light without the aid of co-catalysts. To the best of our knowledge, this is the first report on the synthesis of CuCo2S4 yolk-shells and applications in visible-light-driven photocatalysts.
2. Experimental Section
In a typical synthesis, 35 mg of Cu (NO3)2·3H2O, 72 mg of Co (NO3)2·6H2O was dissolved in a mixture of 7 mL of glycerol and 40 mL of isopropanol to form a clear solution. Then the solution was stirred for 1 h at room temperature and transferred into a Teflon-lined autoclave vessel and kept at 180 °C for 6 h in a muffle furnace. After cooling, the brown precipitate was washed thrice with ethanol and dried in a vacuum oven at 70 °C for 2 h and named as copper-cobalt glycerate precursor (Cu-Co glycerate). For the preparation of CuCo2S4 yolk-shell architectures, 30 mg of the Cu-Co-glycerate precursor was re-dispersed in 20 mL of ethanol solution, followed by the addition of 60 mg of thiourea. Then the mixture was transferred into a Teflon-lined autoclave and heated to 200 °C for 2 h. Finally, the black color product was washed with acetone several times, to obtain the CuCo2S4 (named as amorphous CuCo2S4). To improve the crystallinity, the final product was calcined at 300 °C for 30 min under air atmosphere (named as crystalline CuCo2S4).
Materials Characterization
Crystallinity and phase purity were examined by X-ray powder diffraction (X’pert-PRO-PANalytical X-ray diffractometer operated at 40 Kv). The microstructures and morphologies of the CuCo2S4 were characterized using a scanning electron microscope (SEM: Zeiss EVO 18 electron microscope, Germany) and transmission electron microscopy (TEM: JEOL-JEM 2100, USA). Elemental mapping of the yolk-shell architectures was analyzed using the EDX attached to the TEM instrument. The UV-vis diffuse reflectance spectra (DRS) were analyzed using a JASCO spectrophotometer (V-750, Japan), using BaSO4 as a reference. The photocurrent measurements were recorded using a CHI660B workstation with a three-electrode configuration system. Then, 0.25 M Na2SO4 electrolytewas used for photocurrent measurements. The photocatalytic degradation of MB aqueous dye was carried out at room temperature under the visible-light irradiation of a 300 W tungsten halogen lamp. Then, 50 mg of catalyst and 50 mL of MB solution (10 ppm) was used for the photocatalytic degradation. At given intervals of illumination, the samples of the reaction solution were taken out, centrifuged, and analyzed using the JASCO UV-vis spectrophotometer.
3. Results and Discussion
The XRD pattern (Figure 1a) shows that all the diffraction peaks can be matched to the cubic phase of CuCo2S4 (crystalline) with JCPDS card No. 42-1450 [7]. Any other impurity peaks and secondary phases were observed, indicating that the Cu-Co-glycerate precursor was completely transferred to the CuCo2S4 phase after the sulfidation process with thiourea. According to the Scherrer calculation, the average crystalline size of CuCo2S4 was calculated to be 12 nm. The XRD pattern of amorphous CuCo2S4 (without calcination) did not show any prominent peaks indicating the poor crystalline nature of the material. Figure 1b shows the UV-vis DRS patterns of as-prepared CuCo2S4, which provides imperative evidence of their visible light photocatalytic performance. Apparently, the CuCo2S4 sample exhibited strong photo absorption in the entire visible light region. Using the Tauc plot of (αhν)1/2 vs. photon energy (hν), the band gap value for the CuCo2S4 yolk-shell was calculated to be 1.41 eV, respectively. SEM analysis was employed to investigate the morphology and the detailed structural property of the CuCo2S4 yolk-shells. SEM images from Figure 2a indicating a well-preserved spherical morphology with average diameters of about 1µm were observed. The interior structure of the yolk-shell structure was further investigated by TEM analysis. As shown in Figure 2d,e, the TEM images revealed that the CuCo2S4 composed of many hollow spherical shells with a relatively darker core could be observed in each of the spheres (Figure 2c). Moreover, the amorphous CuCo2S4 did not show any uniform yolk-shell formation. Furthermore, the selected area electron diffraction (SAED) pattern (the inset of Figure 2e) determined that the yolk-shell CuCo2S4 was existing in polycrystalline nature. The TEM observation clearly confirmed that the as-prepared CuCo2S4 yolk-shells consisted of a highly porous nature which may be beneficial for superior photocatalytic degradation. Furthermore, the EDS (Figure 3a–e) images clearly indicate that the Cu, Co, and S elements are uniformly distributed in the CuCo2S4 yolk-shells, as in Reference [8]. These unique yolk-shell structures possessed a porous structure with a large specific surface area, guaranteeing a large contact area between the dye and the photocatalyst. Moreover, the electron separation and transporting behavior of the excited electron-hole pairs in CuCo2S4 could be validated by photocurrent studies. An appreciable photocurrent value can generally originate from the enhanced charge transportation and separation efficiency of photo-generated carriers [9]. As outlined in Figure 3f, the CuCo2S4 yolk-shells show an obvious photocurrent value, which implies that the effective charge separation in the CuCo2S4 system may beneficial for superior photocatalytic activity.
Figure 1.
X-ray diffraction (XRD) patterns of (a) crystalline and amorphous CuCo2S4 (b) UV–vis diffuse reflectance spectra and (αhν)2 versus hν plots of crystalline CuCo2S4.
Figure 2.
(a) Scanning electron microscopy (SEM) images (b) EDS spectra of CuCo2S4 yolk-shell structure (c) Transmission electron microscopy (TEM) images of amorphous CuCo2S4 (d,e) crystalline CuCo2S4 yolk-shell.
Figure 3.
(a–e) EDS mapping (f) Photocurrent studies of CuCo2S4 yolk-shell structure.
Photocatalytic properties of the CuCo2S4 sample were investigated using the degradation of methylene blue (MB) dye as a target pollutant, Figure 4 shows the photocatalytic degradation curves (Ct/C0) in % of MB aqueous dye solution with crystalline and amorphous CuCo2S4 as visible-light photocatalyst. For the blank test without the aid of any photocatalysts, the concentration of MB dye was not changed during the entire period of visible-light irradiation. After adsorption-desorption attainment in the dark, the change in the concentration of MB dye was only about 16% for crystalline CuCo2S4 material which was higher than that of amorphous CuCo2S4 powder (about 8%). However, the visible-light degradation of the crystalline CuCo2S4 was 95% after the 45 min visible-light irradiation, whilst that for the amorphous CuCo2S4 photocatalyst degraded only 38% after 45 min light irradiation [10,11,12]. Hence, crystalline CuCo2S4 had a higher photocatalytic activity than amorphous CuCo2S4 towards the MB degradation due to its pronounced oxygen vacancy and higher surface area (Figures S1 and S2).
Figure 4.
Photodegradation of MB with amorphous and crystalline CuCo2S4 under visible-light irradiation.
As shown in Figure 5a, CuCo2S4 was evaluated by varying the photocatalyst loadings from 25 to 75 mg at 10 mg L−1 of MB concentration. Initially, the degradation efficiency was increased with an increased number of catalytic loadings, which may be due to the availability of active sites for electron-hole pair generation. Beyond the 50 mg of photocatalyst loadings, the degradation efficiency was comparatively lower than the 50 mg loadings, which may be due to reduced light penetration in the photocatalyst system. The effect of dye concentration on the photocatalytic properties of CuCo2S4 was studied by varying the concentrations from 5 mg L−1 to 20 mg L−1, as shown in Figure 5b. It was observed that 5 mg L−1 of MB dye was completely degraded within 60 min. Beyond 10 mg L−1, the degradation efficiency of CuCo2S4 was much lower, which may be due to higher concentration of dye molecules blocking light penetration in the photocatalytic system. Figure 5c shows that the degradation rate constant of MB over the mg loading of CuCo2S4 (25), CuCo2S4 (50), and CuCo2S4 (75), was 12, 15, and 25 min−1 × 10−4, respectively. Hence, the proper loading amount of CuCo2S4 (50%) photocatalytic showed higher photocatalytic activity than other loadings. In addition, as shown in Figure 6, the cycle test results illustrate that the crystalline CuCo2S4 had a lower loss in its activity after three cycles [13,14,15,16,17,18,19,20]. Therefore, crystalline CuCo2S4 yolk-shells powder would be an ideal candidate for visible-light photocatalytic applications. Some few examples of copper based photocatalyst materials and its comparison with the CuCo2S4 yolk-shells are shown in Table 1.
Figure 5.
(a) Photodegradation of MB dye under different amounts of crystalline CuCo2S4 (b) different concentration of MB dye on CuCo2S4 (50 mg). (c) Degradation rate constant of MB over the CuCo2S4 yolk-shells loading.
Figure 6.
Cycle runs of MB photocatalytic degradation in the presence of crystalline CuCo2S4.
Table 1.
Summary of photocatalytic performance of copper based photocatalyst materials.
| S.No | Compound | Synthesis Method | Light Source | Dye | Conc mg L−1 | Catalyst Dosage | Irradiation Time | Efficiency | Ref. |
|---|---|---|---|---|---|---|---|---|---|
| 1 | Cu2SnS3 | Solvothermal | 100 W Xe Lamp | Methylene Blue | 5 | 20 mg | 240 min | N/A | [21] |
| 2 | Cu2SnS3 | Solvothermal | 150 W Tungsten–Halogen Lamp | Eosin | 7.5 | 100 mg | 140 min | N/A | [22] |
| 3 | Cu2SnS3 | Hydrothermal | 500 W Xe Lamp | Rhodamine B | 10 | 100 mg | 210 min | 50% | [23] |
| 4 | CuCo2S4 | Hydrothermal | 500 W Tungsten–Halogen Lamp | Malachite Green | 10 | 50 mg | 360 min | 40% | [24] |
| 5 | CoS2 | Hydrothermal | 8 W Halogen Lamp | Methylene Blue | 5 | 50 mg | 120 min | N/A | [25] |
| 6 | Hexagonal Cu2S copper sheets | N/A | 300 W Xe Lamp | Rhodamine B | 10 | N/A | 60 min | 96% | [26] |
| 7 | Yolk-shell CuCo2S4 | Ion exchange route | 300 W Tungsten Halogen Lamp | Methylene Blue | 10 | 50 mg | 60 min | 95% | This work |
4. Conclusions
In summary, a simple solvothermal route was implemented for the preparation of CuCo2S4 yolk-shell structures. The UV-DRS spectra showed that the CuCo2S4 architectures had a broad visible-light absorption spectrum. The prepared CuCo2S4 yolk-shell structure exhibited good visible-light response and excellent photocatalytic activity towards the degradation of MB dye. The photocatalytic performances of the CuCo2S4 architectures were better than the previously reported degradation rate, which infers the potential applications of CuCo2S4. These results provided new insights that might lead to the development of CuCo2S4 yolk-shells for further application in the field of environmental remediation and energy storage devices, to utilize solar energy effectively.
Acknowledgments
This work was funded by the Prominent Talent Project, Hebei University of Environmental Engineering (BJRC201701), the Project of Natural Science Foundation of Hebei Province (E2016415004, E2016415002), the Project of Science and Technology, Department of Hebei Province (15213629, 15213620), and the scientific research Project item of Hebei province education office (QN2016032).
Supplementary Materials
The following are available online at http://www.mdpi.com/1996-1944/11/11/2303/s1, Figure S1: BET spectrum of CuCo2S4 yolk-shells; Figure S2: XPS spectrum of CuCo2S4 yolk-shells; Figure S3: FT-IR spectrum of CuCo2S4 yolk-shells; Figure S4: SEM, TEM and EDX of amorphous CuCo2S4.
Author Contributions
Y.C., X.J. conceived, designed the experiments and wrote the paper, V.S. and B.P. analyzed the data and analysis tools.
Funding
This research received no external funding.
Conflicts of Interest
The authors declare no conflict of interest.
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