Abstract
A simple and potentially scalable sub- and super-critical methanol technique was applied to synthesize cuprous oxide. Cu2O microcrystals with two morphologies were obtained in methanol of subcritical domain by adjusting the feeding methods. The effects of the reaction time, temperature, pressure, and feeding method on the formation of Cu2O microcrystals were investigated. XRD, SEM, and XPS were applied to analyze the composition and morphology of products. Results showed that pure cuprous oxide could be obtained in subcritical methanol of 230 °C, 7.8 MPa for 15 min. The two as-obtained products displayed octahedral and cubic morphology with an average edge length of 4 and 2 μm by solution and solid feeding methods, respectively. The formation and crystal growth mechanism of Cu2O in subcritical methanol were also proposed on the basis of above results. Furthermore, the two microcrystals were employed as catalysts in the photodecomposition of negatively charged molecule methyl orange. Results showed that both microcrystals possessed excellent photocatalytic activities. However, the obvious difference between cubic and octahedral in photocatalytic performance was not found in the scale of micrometer (2–4 μm).
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Introduction
Cu2O, with a bulk direct band-gap energy of 2.17 eV, is an attractive p-type semiconductor [1]. It has attracted much interest recently due to its excellent catalytic, electrical, sensing, and conductive properties and has been widely applied in various fields, including organic synthesis [2–4], photocatalysis [5–7], solar energy conversion [8], gas sensors [9, 10], lithium ion batteries [11–13], antibacterial [14, 15], and often used as hybrid by compounding with other materials [16–19].
To date, the synthetic strategies of Cu2O nano/micro particles have been developed by many researchers, and various morphologies have been obtained. Among them, the wet chemical approach was the most commonly used method. For instance, the Huang group synthesized Cu2O nanocubes, octahedra, octapods, rhombic dodecahedron, edge- and corner-truncated octahedron, truncated rhombic dodecahedron, etc., by using aqueous solution reduction methods [3, 20–23]. Xu et al. used ascorbic acid as the reducing agent and beta-cyclodextrin as the capping agent to prepare porous Cu2O nanospheres via a sonochemical route [24]. Zhang et al. obtained Cu2O hollow spheres with thin shells in deionized water by using poly(vinylpyrrolidone) as the template, in which, CuAc2·H2O was reduced by ascorbic acid in the presence of PVP and sodium hydroxide [25]. Jin et al. fabricated Cu2O nanowires and nanotubes by reducing Cu2+ with glucose or fructose via Fehling’s reaction [26]. In addition, solvothermal [5, 6, 15, 27] was also often applied to synthesize various interesting cuprous oxide.
In these above reported methods, the morphologies of cuprous oxide nano/micro particles could be easily controlled by adjusting the amount of reductants and surfactants, the introduction order of the reagents, and the reaction time. However, a very complex reaction system consisting of solvent, precursor, reducing agent, surfactant, stabilizer, and other additives was required in these methods. Moreover, these methods were not environmentally friendly due to the usage of toxic agents and expensive organic compounds, which were the major drawbacks for industrial application. Thus, it is urgent to develop a simple, environmentally friendly, and scalable methodology for the synthesis of cuprous oxide.
In recent years, the synthesis of metal oxide nano/micro particles in sub- and super-critical fluids has been extensively reported. Due to the advantages of possessing adjustable physical properties, being environmentally benign and avoiding the usage of toxic and expensive chemical agents, sub- and super-critical fluids have been considered as a promising alternative method for fabricating fine metal-based materials. So far, various metal-based nano/micro particles have been synthesized in sub- and super-critical fluids, such as metal (Cu, Ni, Ag, Co, Au, Pd, Pt) [28–34], metal oxides (Al2O3, TiO2, Ga2O3, CeO2, Fe3O4, ZnO, In2O3, Mn3O4, Gd2O3, Eu3O3, Nd2O3, CuO, Fe2O3, NiO, ZrO2) [31, 32, 35–41], composite metal oxides (BaTiO3, MnFe2O4, Li4Ti5O12, LiFePO4, LiFePO4) [42–45], metal nitride (Cr2N, Co2N, Fe4N, Cu3N, Ni3N) [32], metal sulfide (ZnS, CdS, PbS) [31], and selenides (ZnSe, CdSe, PbSe) [31]. In these studies, methanol, ethanol, water, and CO2 were used as solvents in the formation of sub- and super-critical fluids. Among them, alcohols exhibited greater advantages than water and CO2 due to the more moderate conditions and simpler process. In addition, supercritical or subcritical alcohols technique could also be easily scaled up via a continuous flow type system [29, 35, 38, 39, 46].
To our knowledge, there is no report on the synthesis of cuprous oxide as the only product through sub- and super-critical alcohols. In this paper, we report a simple and scalable method for the synthesis of Cu2O microcrystals with given morphologies in subcritical methanol by using inorganic copper salt as the precursor. Octahedral and cubic cuprous oxide microcrystals were obtained and applied as photocatalyst to degrade methyl orange. The influence of morphology on catalysis performance was also investigated.
Materials and methods
Synthesis of cuprous oxide
For solution feeding methods, typically, 4 g of Cu(NO3)2. 3H2O was dissolved in 30-mL methanol firstly and then introduced into a high-pressure tank reactor (150 mL) purged previously with nitrogen for several minutes. The system was heated to 200–250 °C within 15 min and kept for 15–30 min. In the process, the pressure of the system was 5.6–10 MPa. Upon the completion of the reaction, the reactor was immediately quenched with cold water. The precipitates were filtrated and washed with deionized water and methanol three times to remove the residues. Then, the products were dried in a vacuum oven for 24 h. All of the above reagents were purchased from Sinopharm Chemical Reagent Co, Ltd. (Shanghai, China) and were used without further purification.
For solid feeding methods, 4 g of Cu(NO3)2·3H2O was introduced into the reactor firstly. After being tightly sealed, the air inside was replaced with N2 for several minutes and then the N2 was exhausted under vacuum for 10 min. 30-mL methanol was then discharged into the reactor. The reactor was heated to 230 °C within 15 min and kept for 15 min under the pressure of 7.8 MPa. Subsequent steps are the same with above process.
Characterizations
The particles were characterized by using XRD, SEM, and XPS. XRD patterns of the samples were conducted with an Empyrean X-ray generator (PANalytical B.V., Netherlands). The microscopic feature of the products was observed by scanning electron microscopy (SEM, S-4800 FESEM, Hitachi Ltd, Japan). X-ray photoelectron spectroscopy (XPS, ESCALAB250, Thermo VG, USA) was employed to analyze the surface of transition metal oxides powders.
Photocatalytic performance of cuprous oxide
To investigate the photocatalytic performance of the octahedral and cubic Cu2O microcrystals, methyl orange (MO) (Sinopharm Chemical Reagent Co, Ltd.) was used as a model pollutant. The LED was used as a light source to provide irradiation. 0.1 g of the as-obtained cuprous oxide was dispersed in 100 mL of 10 mg/L aqueous methyl orange solution in a quartz beaker. The solution was then stirred constantly under dark conditions for 60 min to ensure the adsorption/desorption equilibrium between MO and Cu2O. The mixture was then irradiated with visible light irradiation under constant stirring for different time. 1 mL of the sample solution was withdrawn after irradiating at a certain intervals and taken to be detected by a UV–Vis absorption spectrometer (UV-5200, metash instruments Co, Ltd. Shanghai, China) after being treated typically.
Results and discussion
Characterization of synthesized samples
The XRD patterns as illustrated in Fig. 1 showed the crystal phase of samples synthesized in sub- and super-critical methanol with different temperatures and pressures for 30 min by using solution feeding method. All diffraction peaks in Fig. 1a could be indexed to the phase of CuO when the process was carried out under lower temperature (200 °C) and pressure (5.6 MPa). When the temperature and pressure were raised to 230 °C and 7.8 MPa, a mixture of CuO, Cu2O, and Cu was obtained (Fig. 1b), while pure copper was formed under higher temperature (250 °C) and pressure (10 MPa) (Fig. 1c). The above results indicated that only moderate reaction condition (i.e., 230 °C, 7.8 MPa in Fig. 1b) was conductive to the formation of cuprous oxide. Moreover, Fig. 1b shows that there was a large amount of elemental copper, and only a small amount of Cu2O in the mixture, which was supposed to be caused by long reaction time. Thus, the reaction time was shortened to 15 min by keeping the same moderate condition (230 °C, 7.8 MPa). Then diffraction peaks belonging to pure phase of cuprous oxide are observed in Fig. 2a, which could be well indexed to PDF 5-667 with the (224) Pn-3 m space group and a = b = c = 4.27 Å. Six peaks at 2θ = 29.51, 36.38, 42.22, 61.32, 73.48, and 77.26° corresponded to (110), (111), (200), (220), (311), (222) lattice planes of face-centered cubic (fcc) Cu2O structure.
When solid feeding method (in Sect. 2.1) was adopted to synthesize cuprous oxide, pure cuprous oxide could also be obtained (see Fig. 2b) and all diffraction peaks were indexed to PDF 65-3288 with a = b = c = 4.26 Å. Interestingly, however, SEM results showed that the two Cu2O samples synthesized by different feeding methods presented distinct morphologies as shown in Fig. 3. When solution feeding method was applied, the collected samples were octahedral Cu2O with an edge length of 4 μm (Fig. 3a), and when solid feeding method was used, cubic Cu2O with edge length of 2 μm was obtained (Fig. 3b).
The XPS was employed to analyze the surface composition of the Cu2O product and the XPS spectrums of curve fitting of C 1s, N 1s, O 1s, and Cu 2p are shown as Fig. 4. The XPS spectrum was charge corrected to the adventitious C 1s peak at 284.6 eV. The C 1s peak was split into three peaks of 284.5, 285.4, and 287.9 eV, which were ascribed to elemental C, C–OH, and –C=O, respectively (Fig. 4a) [34], while the N 1s peaks in the spectra (see Fig. 4b) could be fitted into four peaks of 396.5, 398.1, 399.7, and 406.5 eV, which were ascribed to nitride, N–O, and NO3 −, respectively [47, 48]. The O 1s peak could be fitted into 3 peaks. The peaks at 529.6, 531.1, and 532.3 were indexed to cupric oxide, cuprous oxide, and –C=O, respectively (Fig. 4c) [21, 34, 49]. In Fig. 4d, the two peaks located at 932.0 and 951.8 eV are assigned to Cu 2p in Cu2O [21], and the six peaks at 933.7, 941. 6, 944.4, 954.0, 961.9, and 963.7 eV correspond to Cu 2p in CuO [49, 50], and peaks located at 935.8 and 956.8 eV are assigned to Cu 2p in Cu(NO3)2 [51]. Both O 1s peak (529.6 eV) and Cu 2p peak in CuO and Cu(NO3)2 indicated that there still was unreduced Cu2+ on the surface of the Cu2O particles. In addition, the generation of –C=O group was confirmed by the peaks at 287.9 eV of C 1s and 532.3 eV of O 1s, which revealed that methanol was oxidized to formaldehyde in the process.
Proposed formation and crystal growth mechanism of Cu2O
For further revealing the formation mechanism of cuprous oxide microcrystals in the subcritical methanol, the following proposed chemical reactions might be involved in the processes:
First, when reaching the subcritical domain, methanol was decomposed into free OH− and CH +3 , and copper nitride was decomposed into copper oxide, nitrogen dioxide, and oxygen, as described in Eqs. (1) and (2), respectively.
Organometallic complex Cu(–O–CH3)OH was synthesized as an intermediate via the collision of methyl cation, hydroxyl anion, and copper oxide. Then, electron transfer from oxygen atoms to copper atoms happened in the organ metallic complex to produce Cu+–OH and methoxy radical (Eq. 3). In Eq. (4), electron was transferred from the O–H bond to O atom to produce Cu+–O and H radical. Cu2O and hydroxyl radical were then synthesized after the continuous electron transferring from Cu+–O radical to Cu and O atom, as described in Eq. (5).
Subsequently, electron transfer in methoxy radicals produced formaldehyde and hydrogen radical (see Eq. 6). At the end of the process, hydrogen radical would react with hydroxyl radical formed in Eq. (5) and unreacted methoxy radical to produce water and methanol, as described in Eqs. (7) and (8).
In addition, the formation mechanism of octahedral and cubic cuprous oxides could be explained according to the crystal growth theory [52], which believed that the morphology of monocrystal was determined by the relative growth rate of different crystal faces. Cu2O belonged to the cubic crystal system, and the evolution of morphology mainly depended on the growth rate of {100} and {111} crystal plane [53]. When {111} facet grew relatively fast, Cu2O crystal tended to form cubic, or else, it tends to form octahedron.
In this study, when solution feeding method was used, Cu(NO3)2 was dissolved adequately in methanol to release abundant NO3 −, which would be adsorbed on the {111} facet of Cu2O nucleation. This adsorption would prevent the crystal growth along the {111} facet, while {100} facet grew relatively faster. As a result, the stable {111} facets were preserved finally to form octahedron. While for solid feeding method, since the concentration of NO3 − in methanol was lower, the growth of {111} facet of Cu2O nucleation was faster than that of {100} facet, which resulted in the elimination of {111} facet and the formation of cubic Cu2O finally.
Photocatalytic performance of cuprous oxides
Octahedral and cubic cuprous oxides were used as a photocatalyst for the decomposition of water containing methyl orange (MO), which was used as a model compound. For comparison, commercially available Cu2O particles were used as control experiment. Figure 5 is the curves of the extent of photodegradation of MO vs. time for the two Cu2O microcrystals as well as the control, dark and blank experiments. It was found that there was no decomposition for MO in dark in the presence of Cu2O. Also no degradation was observed when the solution was placed under radiation but without Cu2O. Moreover, there was also no apparent degradation when using bulk Cu2O as catalyst in control experiment. As expected, both octahedron and cubic cuprous oxide microcrystal were much more photocatalytically active than bulk materials. The degrees of degradation of MO after 6 h of irradiation were 96.5 % and 92.1 % for octahedron and cubic, respectively. However, there was no significant difference in photocatalytic performance between octahedral and cubic. It suggested that in the scale of micrometer (2–4 μm), morphology could not influence the photocatalytic performance.
Conclusion
Octahedral and cubic Cu2O microcrystals with an average edge length of 4 and 2 μm, respectively, were synthesized by a simple and potentially scalable subcritical methanol method. It was concluded that pure phase of cuprous oxides could be obtained in a short reaction time (15 min) under moderate temperature (230 °C) and pressure (7.8 MPa). The feeding method played an important role in the formation process of different morphologies. The oxidation product, formaldehyde, was confirmed to exist on the surface of cuprous oxide, which suggested that the subcritical methanol acted as reaction medium as well as reducing agent in the process. In addition, both octahedron and cubic cuprous oxide microcrystal exhibited morphology-independent and excellent photocatalytic performance in the degradation of methyl orange.
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Acknowledgements
The authors gratefully acknowledge the financial supports by the Scientific Research Starting Foundation for Doctors of Science and Technology Agency of Liaoning Province, China (Grant No. 20111047) and (Grant No. 20121070), and Program for Liaoning Excellent Talents in University (Grant No. LR2012012) and (Grant No. LJQ2012034).
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Li, S., Ge, X., Jiang, S. et al. Synthesis of octahedral and cubic Cu2O microcrystals in sub- and super-critical methanol and their photocatalytic performance. J Mater Sci 50, 4115–4121 (2015). https://doi.org/10.1007/s10853-015-8967-3
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DOI: https://doi.org/10.1007/s10853-015-8967-3