Kesheng Caoa,
Xueyu Gea,
Shuang Lia,
Zhengshan Tian*a,
Suya Cuia,
Guijin Guoa,
Liuqing Yanga,
Xingwu Lia,
Yabo Wanga,
Suzhen Baia,
Qian Wei*b and
Wei Li*b
aSchool of Chemistry and Environmental Engineering, Henan Province Engineering Technology Research Center of Green Hydrogen & Electrochemical Energy Storage, Pingdingshan University, Pingdingshan, 467000, China. E-mail: tianzhengshan@163.com
bCollege of Optical, Mechanical and Electrical Engineering, Zhejiang A&F University, Hangzhou, 311300, China. E-mail: qweiyk@126.com; liuwei@zafu.edu.cn
First published on 21st May 2025
Graphene-based and g-C3N4-based nanocomposites can effectively remove organic pollutants from water. However, the reasonable design and scale preparation of hybrid nanomaterials of reduced graphene oxide (rGO), g-C3N4 and silver nanoparticles (Ag NPs) with improved performance for practical application need to be further explored. Herein, a 3D rGO/g-C3N4 nanocomposite loaded with Ag NPs was successfully fabricated through a facile three-step synthetic route. The microstructure and morphology of GO, g-C3N4, rGO/g-C3N4 and rGO/g-C3N4 nanocomposite loaded with Ag NPs were characterized and analyzed. The experimental results show that the as-prepared nanocomposite loaded with Ag NPs has excellent activity to remove methylene blue (MB) from water under visible light irradiation, and its maximum removal capacity is high as 49.60 mg g−1 within 60 min. Based on its possible catalytic process and kinetic analysis, the adsorption and catalytic performance of this nanocomposite may be attributed to a synergistic effect of rGO, g-C3N4 and Ag NPs. In addition, it can provide a useful reference for the rational design and scale preparation of rGO/g-C3N4 nanocomposite for practical applications.
On the one hand, graphene as a 2D nanocarbon material, has lots of novel functional applications due to its high strength, high conductivity and large specific surface area and so on.8–10 Graphene-based nanomaterials are generally used as excellent adsorbents and catalysts owing to their excellent physical and chemical properties.11–14 However, graphene has no functional groups (such as carboxyl group, hydroxyl group and epoxy group) on its surface, and van der Waals forces lead to easy agglomerate between different layers,15,16 thus it is very difficult to interact with other molecules or ions, which hinders its practical functional application.
On the other hand, graphene oxide (GO), as a derivative of graphene, has some advantages such as rich pore structure and some oxygen-containing groups on its surface.17–19 Importantly, these oxygen-containing groups can provide numerous reactive sites to enhance interactions with other molecules or ions.20–22 Moreover, the negatively charged GO with excellent hydrophilicity can strongly adsorb heavy metal cations and cationic dyes in wastewater through electrostatic actions and π–π interactions.23–25
At the same time, to improve the adsorption and catalytic performance of GO, it is usually hybridized to prepare GO-based nanocomposites, especially nanomaterials hybridized with Ag NPs have attracted intense attention because of their excellent performance.26–28 For example, Rath and co-workers28 designed GO/Ag nanocomposite to adsorb crystal violet dye at pH of 8, and the maximum adsorption capacity of crystal violet was as high as 48.78 mg g−1. Moreover, after many adsorption and desorption cycles, its recyclability and stability were also satisfactory. Naeem and co-workers4 prepared GO/Ag nanocomposite not only as adsorbent to adsorb multiple pollutants, but also as catalyst to catalyze the degradation of dyes. Mohamed and co-workers29 designed rGO impregnated with Ag NPs to catalyze the degradation of MB, and this nanocomposite of rGO with Ag NPs was efficiently used as adsorbent and catalyst to remove organic dyes because of its excellent electrical conductivity and highly catalytic active feature of Ag NPs.
Recently, graphitic carbon nitride (g-C3N4), as a novel 2D graphene analogue, has emerged as a promising photocatalyst since 2009 (ref. 30) due to its excellent physical and chemical properties such as tunable band structure, non-toxicity, facile synthesis and chemical stability.31–33 However, the pristine g-C3N4 catalyst still has some inherent disadvantages such as its poor charge separation, limited light absorption and low surface area, thus leading to its moderate photocatalytic activity.34–36
To improve the photocatalytic performance of g-C3N4-based photocatalysts, some further modification strategies (such as vacancy engineering, nanostructure design, heteroatom doping and forming heterostructure) have been attempted.37 Particularly, g-C3N4 with 3D nanostructure can increase the specific surface area and improve the anchoring stability of cocatalysts. Moreover, graphene with 3D nanostructure can promote light absorption and enhance charge migration.38 because graphene acts as a light-transmitting material and a conductor.39 At the same time, the loaded cocatalysts can be used as the electron acceptors to remarkably promote the electron–hole separation.37
More recently, many efforts have been focused on the internal electrons of g-C3N4 at the atomic scale through monatomic engineering.40–43 The metal atoms can be uniformly anchored on the network by forming coordination bonds with lone pair electrons of the nitrogen contained in g-C3N4. Specifically, Ag NPs dispersed in the g-C3N4 nanosheets can significantly accelerate the charge separation to improve the photocatalytic activity.44,45 For example, Jiang and co-workers40 designed the g-C3N4 catalyst anchored with Ag NPs, which exhibited excellent catalytic activity and durability for efficient photocatalytic hydrogen evolution, because the Ag NPs not only extend the visible light absorption region but also facilitate electron transfer.41–43
Although numerous results of g-C3N4-based photocatalysts have been achieved, however, to overcome their serious drawbacks such as small specific surface area, fast charge recombination and limited visible-light absorption,46,47 the reasonable design of g-C3N4-based photocatalysts with rGO and Ag NPs is still a research hotspot. In particular, Ag doping can not only enhance the light absorption but also accelerate the photogenerated carrier transfer process, and its related mechanism needs to be given intensified attention. Therefore, the reasonable design and scale preparation of hybrid nanomaterials of rGO, g-C3N4 and Ag NPs with improved performance for practical applications need to be further explored.
In this paper, we successfully fabricated a 3D rGO/g-C3N4 nanocomposite loaded with Ag NPs (rGO/g-C3N4/Ag NPs) through a facile three-step synthetic route. At the same time, the adsorption and catalytic properties of this nanocomposite were analyzed. Moreover, its possible catalytic process and kinetic analysis were discussed.
On the basis of the as-prepared GO and g-C3N4 suspension, GO nanosheets with excellent hydrophilicity can be evenly dispersed in an aqueous solution, and they are beneficial to interact with g-C3N4 nanosheets to form GO/g-C3N4 nanocomposite.53,54 Moreover, during the hydrothermal reaction, GO and g-C3N4 nanosheets can be self-assembled to rGO/g-C3N4 nanocomposite with 3D network structure, similar to the self-assembly of GO nanosheets.55
The rGO/g-C3N4/Ag NPs mainly consists of three active ingredients (rGO, g-C3N4 and Ag NPs), which are effectively combined together. Each of them has a very important role in the nanocomposite for functional applications, and thus each ingredient needs to be considered in the preparation process in detail.
Based on the improved Hummers' method18,19,48 and subsequent ultrasonic stripping,49–51 the graphite powders were converted into GO sheets, accompanied with a slight color changing from dark black to grey black, as shown in Fig. 2a and b. The obtained GO sheets are single layer or several layers with loose, stacked and cross-linked structure, as displayed in Fig. 2c and d.
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Fig. 2 Optical photos of graphite powders (a) and GO powders (b). SEM image of GO nanosheets (c) and TEM image of GO nanosheets (d). |
The microstructure of g-C3N4 powders was shown in Fig. 3. The melamine powders were transformed into g-C3N4 powders after a thermal polymerization reaction of 550 °C for 5 h in a covered porcelain crucible. Moreover, the colors of the samples change from cream white color of melamine powders to light yellow color of g-C3N4 powders, as shown in Fig. 3a and b. Seen from SEM images in Fig. 3c, the g-C3N4 powders consist of numerous nanosheets with mixed lamellar and stacked structure. In particular, the micromorphology and size of the g-C3N4 nanosheets are more uniform after ultrasonication, as shown in Fig. 3d.
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Fig. 3 Optical photos of melamine powders (a) and g-C3N4 powders (b). SEM images of g-C3N4 powders (c) and g-C3N4 sheets (d). |
During the preparation of rGO/g-C3N4/Ag NPs, an aqueous solution of glucose (5 wt%) was slowly added into a dispersion of rGO/g-C3N4 and silver ammonia solution, and then [Ag(NH3)2]+ was reduced by the green reducing agent of glucose under 70 °C water bath.
When the above hybrid mixture was remained static for 20 min, such that a bright silver mirror was attached onto the inside of the beaker, as shown in Fig. 4a. Interestingly, the ultrasonic treatment was instead of resting state, [Ag(NH3)2]+ was reduced not to form bright and uniform silver mirror, but to load into the rGO/g-C3N4 nanocomposite as Ag NPs, as shown in Fig. 4b.
As a contrast, without the rGO/g-C3N4 nanocomposite as a load carrier, the Ag NPs were prepared under 70 °C water bath and ultrasonic treatment, and the microstructure of Ag NPs was analyzed by SEM and TEM. The obtained results show that the particle sizes of Ag NPs are 50–100 nm, as shown in Fig. 4c and d. In the formation process of Ag NPs without a carrier, the sizes of Ag NPs are not uniform, which may be attributed to some influencing factors such as agglomeration, surface coatings and overlapping.
Compared with g-C3N4 sheets in Fig. 3d, the rGO/g-C3N4 nanocomposite presents a 3D porous structure, which can effectively increase specific surface area and adsorption capacity, as shown in Fig. 5a and b. At the same time, the rGO/g-C3N4 nanocomposite was successfully prepared in a high-pressure reactor at 200 °C for 5 h, thus some oxygen-containing groups were removed from the GO surface. Moreover, the electrical conductivity of rGO sheets will be greatly improved, as well as rGO and g-C3N4 sheets are tightly bonded and their π–π interactions has been strengthened, which are beneficial to promote the electron–hole separation.
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Fig. 5 SEM images of rGO/g-C3N4 nanocomposite with different magnifications (a and b), and rGO/g-C3N4/Ag NPs with different magnifications (c and d). |
As shown in Fig. 5c and d, the rGO/g-C3N4/Ag NPs has a 3D porous structure, while its microstructure can be further optimized, and numerous of Ag NPs are in loaded onto the surface or into inside of the nanocomposite.
Based on the above prepared GO, g-C3N4 and rGO/g-C3N4, the rGO/g-C3N4 loaded with Ag NPs was rationally constructed. Compared to g-C3N4 sheets in Fig. 3d, the rGO/g-C3N4 nanocomposite presents a 3D porous structure, which effectively increases its specific surface area. Moreover, the hydrothermal reaction caused GO/g-C3N4 to rGO/g-C3N4, and some oxygen-containing groups on GO surface were removed. Compared to rGO/g-C3N4, the rGO/g-C3N4/Ag NPs also presents a 3D porous structure, and its morphology can be further optimized due to in situ loading of Ag NPs, as shown in Fig. 5c and d.
To analyze the composition of rGO/g-C3N4/Ag NPs, its elemental mapping for elements (including C, O, N and Ag) was performed, as shown in Fig. 6. The elemental mappings of a selected region clearly demonstrate the corresponding distributions and atomic percents (C, O, N and Ag atoms).
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Fig. 6 (a) SEM image of rGO/g-C3N4/Ag NPs in a selected region, and (b–e) Elemental mappings of C, O, N and Ag. |
As the same time, FTIR spectra are employed to analyze the functional groups of GO, g-C3N4 and rGO/g-C3N4/Ag NPs. It can be seen from Fig. 7a that the characteristic peaks located at 3000–3500 cm−1 should be caused by the stretching vibration of –OH and –NH2 groups.56,57 While the peaks of 1200–1700 cm−1 are due to the stretching vibrations of CN heterocycles, and the peak of 806 cm−1 is related to the breathing and stretching mode of CN-heterocyclic triazine. As mentioned above, the characteristic peaks of FTIR spectra are completely consistent with the reported literature.56,57
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Fig. 7 FTIR spectra of g-C3N4 sheets prepared at different temperatures (a), and FTIR spectra of GO, g-C3N4 and rGO/g-C3N4/Ag NPs (b). |
The reaction temperature is considered as a crucial influencing factor on the crystallinity of g-C3N4 sheets, which has played an important role on its photocatalytic activity.58 Thus, different reaction temperatures (such as 500 °C, 550 °C and 600 °C) were considered based on the thermal polymerization reaction.52,58 Compared with g-C3N4 sheets prepared at 550 °C and 600 °C, the characteristic FTIR peaks of g-C3N4 sheets prepared at 500 °C are not obvious. Although the peak positions of g-C3N4 sheets prepared at 550 °C and 600 °C are almost no difference, while there are obvious differences in their colors, that is, the color of g-C3N4 sheets at 550 °C is light-yellow and the color of g-C3N4 sheets at 600 °C is deep-yellow.
Seen from the characteristic FTIR peaks in Fig. 7b, the rGO/g-C3N4/Ag NPs contains some oxygen-containing functional groups. The absorption peak around 1600 cm−1 is the basic skeleton of CC bond, and the absorption peak near 1750 cm−1 is the C
O stretching vibration absorption peak, as well as the absorption peak near 3400 cm−1 is the O–H stretching vibration absorption peak.50,51 Therefore, the rGO/g-C3N4/Ag NPs has some functional group structures, which will help it absorb pollutants from water for degradation.
Raman spectra in Fig. 8a show that the characteristic peak near 800 cm−1 corresponds to the bending vibration of the triazine ring, and the characteristic peak near 1600 cm−1 is caused by the stretching vibration of the CN heterocyclic compound.59 The Raman spectral characteristic peaks of g-C3N4 prepared at 500 °C and 550 °C are more obvious compared with that of g-C3N4 prepared at 600 °C. Based on above relevant analysis of FTIR and Raman spectra of g-C3N4 samples prepared 500 °C, 550 °C and 600 °C, the g-C3N4 powders in our experiment were deliberately prepared at 550 °C.52,58
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Fig. 8 Raman spectra of g-C3N4 sheets prepared at different temperatures (a), and GO/g-C3N4, rGO/g-C3N4 and rGO/g-C3N4/Ag NPs (b). |
It can be observed from Fig. 8b that the characteristic peaks near 1350 cm−1 and 1600 cm−1 correspond to the D and G bands of the graphite structure, respectively. Moreover, the ratio of D peak intensity to G peak intensity (ID/IG) is generally used to represent the degree of graphitization of graphite,50 after the hydrothermal reaction of rGO/g-C3N4 and in situ loading of Ag NPs, the value of ID/IG increases from GO/g-C3N4 and rGO/g-C3N4 to rGO/g-C3N4/Ag NPs, indicating that some oxygen-containing groups in rGO/g-C3N4 nanocomposite can be removed by heating reduction50 and the Ag NPs have Raman enhancement effects.60
Seen from XRD analysis in Fig. 9a, there are a weak peak (13.2°) and a prominent peak (27.5°), which corresponds to the (100) and (002) crystal faces of g-C3N4 sheet,52,56 respectively. Moreover, the XRD patterns of g-C3N4 sheets prepared at different temperatures (inset of Fig. 9a) show that the g-C3N4 sheets prepared at 550 °C have more obvious characteristic peaks compared with that of g-C3N4 sheets prepared at 500 °C and 600 °C.
For rGO sheets, the diffraction peak at 10.5° is a characteristic diffraction peak (Fig. 9b) of the crystal face of (001).50,51 Especially, as displayed in Fig. 9c, the diffraction peaks of rGO/g-C3N4 nanocomposite with Ag NPs located at 38.2° (111), 44.5° (200), 64.5° (220) and 77.5° (311) are the characteristic diffraction peaks of Ag NPs (JCPDS No. 04-0783),40,41 respectively, indicating that Ag NPs were successfully introduced into the rGO/g-C3N4 nanocomposite. The diffraction peaks of Ag NPs are strong and there are no other miscellaneous peaks, which confirms the high purity of Ag NPs.40,41
Very significantly, there is a noticeable change after in situ loading of Ag NPs, especially their intensity of the XRD patterns has changed in rGO/g-C3N4/Ag NPs. That is, a prominent peak at (002) and a weak peak at (100) crystal faces of g-C3N4 sheets are shown in Fig. 9a, as well as a prominent peak at (002) crystal face of g-C3N4 sheets and a weak peak at (001) crystal face of rGO sheets are shown in Fig. 9b. However, the diffraction peaks of Ag NPs are very strong, such that the diffraction peaks of g-C3N4 sheets and rGO are too weak to be seen in rGO/g-C3N4/Ag NPs, as shown in Fig. 9c. Moreover, the crystallite size of Ag NPs can play an important role on photocatalytic efficiency. Generally, smaller crystallites imply higher surface-to-volume ratio with enhancing photocatalytic activity.61
Thermogravimetric analysis was performed to calculate the water adsorption capacity of 3D porous structure.62 As the adsorbed water evaporates at room temperature, the weight loss of this nanocomposite is about 56.7 wt%, and then the labile oxygen-containing functional groups are broken down to produce water at around 200 °C, the weight loss of hydrogel is about 20.7 wt%.63
Firstly, the test experiments were carried out under alkaline medium, that is, the pH value of an aqueous solution containing MB was about 8.28 Typically, 100 mg of adsorbent (such as g-C3N4 sheets, rGO/g-C3N4 and rGO/g-C3N4/Ag NPs) was immersed into 100 mL of MB solution (50 mg L−1) in the dark, followed by stirring at 200 rpm at room temperature. At time intervals of 10 min, the adsorbent was separated by filtration and the concentration of residual MB in the filtrate was calculated by Beer's law based on the absorption peak at 662 nm with a UV-visible spectrophotometer (Shimadzu UV-2450).51,63–65
Secondly, under simulated solar irradiation, a light resource was introduced using a 300 W Xe lamp. Typically, 100 mg of adsorbent was immersed into 100 mL of MB solution (50 mg L−1) under simulated solar irradiation, followed by stirring at 200 rpm at room temperature. At time intervals of 10 min, the adsorbent was separated by filtration and the concentration of residual MB in the filtrate was calculated by Beer's law based on the absorption peak at 662 nm with a UV-visible spectrophotometer (Shimadzu UV-2450).51,63–65
Finally, the ratio of temporal concentration to initial concentration (C/C0) was analyzed with the change of adsorption time. The elimination efficiency was assessed by using C/C0, which is equal to A/A0. Where A0 and C0 were the initial absorbance and concentration of MB, respectively. The A and C were the corresponding absorbance and concentration of MB to be tested at different adsorption times, respectively.
As can be seen from Fig. 10a, when the pristine g-C3N4 sheets acts as an adsorbent to adsorb MB from water in the dark, it takes about 60 min to reach adsorption equilibrium and the value of C/C0 decreases to 21.80%. Moreover, the rGO/g-C3N4 nanocomposite acts as an adsorbent, the adsorption reaches equilibrium at 60 min and the value of C/C0 decreases to 15.80%. While the rGO/g-C3N4/Ag NPs is used as the adsorbent, the adsorption equilibrium time is also 60 min and the value of C/C0 decreases to 12.80%.
As a control experiment, the visible light was introduced on the basis of the above same experimental conditions, the pristine g-C3N4 sheets, rGO/g-C3N4 and rGO/g-C3N4/Ag NPs were employed as adsorbents and catalysts, respectively. At equilibrium, their values of C/C0 decrease to 18.80%, 10.80% and 0.80%, respectively, as shown in Fig. 10b.
From the above results, it was reasoned that the pristine g-C3N4 sheets, rGO/g-C3N4 and rGO/g-C3N4/Ag NPs were only employed as adsorbents in the dark, respectively, and their removal capacities (Fig. 10c) were calculated as 39.10 mg g−1, 42.10 mg g−1, and 43.60 mg g−1, respectively. However, as the visible light is introduced, they are not only adsorbents but also catalysts, such that there is a significant decline in their values of C/C0 (from 21.80%, 15.80% and 12.80% to 18.80%, 10.80% and 0.80%), as well as their removal capacities (Fig. 10d) are up to 40.60 mg g−1, 44.70 mg g−1, and 49.60 mg g−1, respectively. Compared with the pristine g-C3N4 sheets and rGO/g-C3N4, the rGO/g-C3N4/Ag NPs has best performance.
Among them, a 3D porous structure of rGO/g-C3N4 nanosheets with rich functional groups provides an effective carrier to hybridize with Ag NPs and adsorb MB, as well as enhance light absorption.39 The rGO nanosheets act as the charge transmission bridge between g-C3N4 nanosheets and Ag NPs, which not only facilitates the separation of electrons and holes but also improves the stability of the photocatalyst of Ag NPs.37,39 The Ag NPs can display a plasmon effect of the localized surface plasmon resonance, such that the Ag NPs not only act as photocatalyst, but also enhance light absorption and promote charge separation.40–45,60
Based on the above analysis, the rGO/g-C3N4/Ag NPs was employed as not only adsorbent but also catalyst under visible light irradiation, and their values of C/C0 decrease from 12.80% to 0.80%, with MB removal capacity increase from 43.60 mg g−1 to 49.60 mg g−1. Under visible light irradiation, the adsorption and catalytic performance of rGO/g-C3N4/Ag NPs is better than that reported in many literature, which is compared with the related reports,51,53,63,64,66,67 as shown in Table 1.
The pH of the system is a very important factor, which influences the photocatalytic degradation activities of the catalysts.28,68 Fig. 11a demonstrates the performance of this catalyst of rGO/g-C3N4/Ag NPs at different pH values towards the degradation of MB. There is a basic tendency to increase catalytic activity as pH increases, reaching a maximum value at pH value of 11.69
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Fig. 11 Photocatalytic degradation of MB under visible light irradiation. (a) Effect of solution pH and (b) stability experiments for MB degradation. |
In our experiment, MB is selected as a model compound that is a cationic dye. Although the pH of the system is a very important factor, at the same time, positively charged ions with strong electrostatic interactions will interfere with the efficiency of the method. Moreover, if some ions get through π–π interactions to compete for active sites on surface of catalyst, they can also interfere with the efficiency of this method.
The stability and reusability of a catalyst is very important for assessing the practical applicability of the catalyst. After a run, the filtered photocatalyst was washed for three times with ethanol and deionized water, respectively, and dried at 80 °C for 5 h. After 4 cycles, the efficiency of this photocatalyst is still more than 90%, as shown in Fig. 11b.
There are three kinds of heterojunctions existing in rGO/g-C3N4/Ag NPs, that is, the heterojunctions exist between rGO/g-C3N4, g-C3N4/Ag and rGO/Ag, and they will play relevant roles in the photocatalytic process. As a typical n-type semiconductor, the g-C3N4 nanosheet can be excited to generate photogenerated electrons and holes under visible light irradiation. In this 3D rGO/g-C3N4/Ag NPs, rGO is not only used to enhance light absorption, but also used as an excellent conductor of electrons to promote the separation of photogenerated electron–hole pairs.53 At the same time, Ag NPs has a strong localized surface plasmon resonance effect under visible light irradiation, which not only enhances light absorption, but also increases the generation rate of photogenerated electron–hole pairs on the surface of g-C3N4.40,41,44,45,54 In the 3D network structure, rGO, g-C3N4 and Ag NPs play an effective synergistic role to overcome the drawbacks of g-C3N4-based photocatalyst such as small specific surface area, fast charge recombination and limited visible-light absorption. Thus the photogenerated electrons generated by g-C3N4 nanosheet under the excitation of visible light can effectually react with O2 to form the active species ·O2− to catalyze the decomposition of MB.
Based on the above photocatalytic analysis and the mechanism proposed, the kinetic of adsorption and degradation of MB belongs to pseudo-first order kinetics.34,54,68 Under visible light irradiation, the reaction rate constants of g-C3N4 sheets and rGO/g-C3N4 were calculated as 0.02622/min and 0.03608/min, respectively. While the reaction rate constant of rGO/g-C3N4/Ag NPs was calculated as 0.07795/min, which is higher than that g-C3N4 sheets and rGO/g-C3N4.
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