Faramarz Safari,
Reza Poursalehi* and
Hamid Delavari
Nanotechnology Group, Faculty of Engineering and Technology, Tarbiat Modares University, Tehran, Iran. E-mail: poursalehi@modares.ac.ir
First published on 27th August 2024
Graphitic carbon nitride (g-C3N4) nanostructures were synthesized via the calcination of urea at various temperatures ranging between 400 and 600 °C and were utilized for photoreduction of Cr(VI) in aqueous medium. Due to the low adsorption of Cr(VI) on the g-C3N4 surface, a more accurate assessment of the photocatalytic performance of the samples was carried out. Although the characterization showed that the specific surface of samples increased as the calcination temperature increased, the most efficient product in terms of the photoreduction duration of Cr(VI) was produced through the calcination process carried out at 450 °C, which reduced the concentration by more than 99% in 40 minutes. These results demonstrate that the structural and surface properties of g-C3N4 are critical factors that impact the photocatalytic performance. Alongside the calcination temperatures, the concentration of citric acid as a hole scavenger, the source of illumination, pH levels, and the recycling ability of the produced specimen at 450 °C were also investigated. Conspicuously, the photocatalyst works better when more citric acid is present and the pH level decreases. Out of all the cases studied regarding the light source, the 400 nm LED light source was found to be the most efficient. Additionally, even after going through the photoreduction process four times, the photocatalyst still remained highly efficient.
Extensive research has been conducted on renewable, cost-efficient, eco-friendly and highly efficient photocatalytic reactions for the purpose of reducing organic pollutants or heavy metals.9,10 In the past few decades, several materials including TiO2, ZnO, WO3, CdS, Bi2S3 and Fe2O3 nanostructures have been reported to exhibit photocatalytic properties.11–15 Over the past decade, significant interest has been devoted to graphitic carbon nitride (g-C3N4), which is a metal-free polymeric two dimensional (2D) semiconductor that has a narrow band gap that enables effective visible light absorption.16 g-C3N4 is a π-conjugated polymeric n-type semiconductor, with its two chemical structures depicted in Fig. 1.17,18 Moreover, the distinctive characteristics of g-C3N4, such as its low cost and straightforward synthesis, the potential for adjustability and resistance to thermal and chemical degradation, have garnered significant attentions as a research target within the realm of photocatalysis.19 Numerous investigations have additionally directed attention towards the amalgamation and arrangement of g-C3N4 with other semiconductors to refine properties and conduct band gap engineering, as evidenced by a range of studies.20–22
Various organic precursors, including cyanamide, dicyanamide, melamine, urea and thiourea, have been employed in the synthesis of g-C3N4 through polymerization reactions.23 Calcination at atmospheric pressure is a commonly utilized method that is fairly easy to perform in a furnace. The properties of the resultant product are greatly influenced by the conditions under which the heating is conducted, such as the heating rate from room temperature, along with the duration and temperature of the calcination process. Various photoreactions were utilized to investigate the property disparities of g-C3N4, which was synthesized employing different precursors under diverse conditions. The investigation of calcination temperature has been a prevalent parameter for various chemical reactions, including CO2 conversion, H2 production, NO oxidation and dyes photodegradation, such as those observed in methylene blue, methyl orange, rhodamine B and murexide.24–30 Moreover, analogous photoreactions have examined the impact of various factors on the outcome of the reaction, including the precursor substance, heating rate, and duration of calcination.31–33
Investigation of the g-C3N4 efficiency with Cr(VI) photoreduction, besides having environmental benefits, can help to better understand the photoactivity of g-C3N4 because of the very insignificant adsorption of Cr(VI) on the g-C3N4 surface. Based on the results of studies on the effects of calcination temperature, the specific area of g-C3N4 increases as the calcination temperature increases.25,26 The establishment of the adsorption–desorption equilibrium is a common step before the irradiation of the light source in photoreaction experiments and it has also an effect on the reaction kinetics.34 In addition, due to the adsorption of dyes on the g-C3N4 surface, the dye removal efficiency in the adsorption–desorption equilibrium step has been increased by surface area increase. This issue causes different mass transfer conditions at the irradiation step beginning including concentration discrepancy in solution and different concentration gradian in the binary layer on the photocatalyst surface.35 As well as dye adsorption on the photocatalyst surface can affect light adsorption.36 The effect of precursors on g-C3N4 in the photoreduction of Cr(VI) has been studied by Liang et al. and urea has performed the best efficiency between dicyandiamide, melamine, thiourea, and urea.37 Furthermore, numerous studies have been conducted on the improvement of g-C3N4 properties by adding various material for better photoreduction of Cr(VI).38,39 Yang et al. studied the composition of g-C3N4 by three metal oxides, including TiO2, Fe3O4@SiO2 by hydro-gel synthesis method which the best performance was seen by the sample that calcinated at 450 °C.40 Wang et al. studied the g-C3N4/ZnS coupled composite synthesized at 600 °C that can reduce more than 90% of Cr(VI) solution with a concentration of 10 mg L−1 in 120 min under 500 W xenon lamp.41 Xiao et al. succeeded in photoreduction of Cr(VI) by adding α-Fe2O3 to g-C3N4 by hydrothermal method.42 By doping Br in the g-C3N4 structure, Wang et al. reduced Cr(VI) with a concentration of 20 mg L−1 by 60%.43 Also, studies have been conducted on the synthesis of MoS2 and WO3 heterostructures with g-C3N4, and these materials have improved the performance of g-C3N4 in removing the Cr(VI).44,45 Adding other semiconductors, including metal oxides, can be a useful solution for band gap engineering as a result of improving photocatalytic performance. On the other hand, the release of these compounds amid the reaction can cause harmfulness and be challenging. Hence, engineering the properties of carbon nitride alone as a metal-free semiconductor can be a great arrangement for the photoreduction of Cr(VI).
Within the present study, the synthesis of g-C3N4 was conducted through the calcination of urea at varying temperatures ranging from 400 to 600 °C for the investigation of Cr(VI) photoreduction performance. The products were subsequently characterized, including their structural, morphological, optical, and photoreduction performance in regard to Cr(VI). To the best of our knowledge, investigating the impact of urea calcination temperature on the performance of g-C3N4 for the photoreduction of Cr(VI) has not been reported so far. The photocatalyst synthesized at 450 °C exhibited superior efficacy in photoreduction, leading to its selection for further assessment with respect to recycling capacity, citric acid level, light source, and pH impacts.
The functional groups and chemical bonds contained in the produced g-C3N4 were investigated through exploration using FT-IR spectroscopy. The outcomes FT-IR spectra can be observed in Fig. 4. The samples exhibit analogous patterns within the spectrum spanning 1200–1650 cm−1, with a discernible increase in the sharpness of the absorption peak observable as the temperature of synthesis was heightened. The spectral peaks located at 808 and 889 cm−1 have been assigned to the breathing mode of tri-s-triazine and the deformation mode of N–H bonds, respectively.47,48 The peaks observed at around 1238, 1313, 1400, 1455, and 1558 cm−1 corresponded to the C–N bond and the peak at 1635 cm−1 was associated with CN stretching vibration mode.49–51 In addition, a broad band in the range of 3000–3500 cm−1 indicates the existence of N–H stretching vibrations.52
The Raman spectra of prepared samples are depicted in Fig. 5. For g-C3N4, several characteristic peaks at 1636, 1586, 1466, 1226, 1153, 988, 763, 704, 584 and 474 cm−1 were identified, aligning to the typical vibration modes of CN heterocycles. Notably, the most intense peak in the g-C3N4 Raman spectra appears at 1586 cm−1 attributed to the ring-valence vibration of species E′. Additionally, the peak at 584 cm−1 in the lower frequency range is also associated with species E′, while the peak at 980 cm−1 corresponds to the breathing 1 mode of the triazine ring.53,54
Fig. 6 depicts the SEM images acquired from the g-C3N4 samples. The images suggest that changes in the morphology are associated with a rise in temperature. The CN400 sample exhibits agglomerations of substances that are merged together. As the temperature approaches 450 °C, the morphology of the particles tends to exhibit a more plate-like geometry with increased intertwining.27 Upon reaching a temperature of 500 °C, smaller particles become evident, whereas exposure to 550 °C leads to the generation of cavities within smaller particles. Upon attaining a temperature of 600 °C, the particles underwent a transformation and assumed the morphology of small plates.55 The thickness of these particles was subsequently determined as 28 ± 1 nm. Also, the outcomes of the EDS analysis conducted on the powders, are presented in Table 1. The results reveal that the weight ratio of carbon to nitrogen elements exhibited an initial increase with rising temperature, followed by a subsequent decrease.
Sample | Product to urea mass ratio (%) | Band gap | BET | EDS atomic ratio (W%) | |||||
---|---|---|---|---|---|---|---|---|---|
Tauc equation | PL (365 nm) | PL (405 nm) | as (m2 g−1) | Pore volume (cm3 g−1) | C | N | C/N | ||
CN400 | 10.42 | 2.75 | 2.86 | 2.86 | 8.89 | 0.006 | 34.43 | 65.57 | 0.53 |
CN450 | 4.63 | 2.65 | 2.79 | 2.81 | 23.68 | 0.181 | 35.08 | 64.92 | 0.54 |
CN500 | 3.96 | 2.59 | 2.70 | 2.70 | 33.53 | 0.217 | 42.24 | 57.76 | 0.73 |
CN550 | 2.87 | 2.65 | 2.70 | 2.70 | 67.44 | 0.524 | 35.56 | 64.44 | 0.55 |
CN600 | 1.42 | 2.89 | 2.77 | 2.73 | 66.84 | 0.688 | 34.13 | 65.87 | 0.52 |
The surface area and porosity of the samples were assessed utilizing N2 adsorption–desorption isotherms. The findings reveal that the samples exhibit an IV adsorption–desorption isotherm displaying a H3 hysteresis loop, indicating the presence of a mesoporous configuration, as illustrated in Fig. 7. The surface area and pore volume of the analyzed specimens were computed and recorded in Table 1, presenting a comprehensive summary of the results. The observed phenomenon may be attributed to variations in the bubbling and oxidation of intermediate compounds that arise during the process of calcination. These outcomes appear to adhere to the morphology alterations that were witnessed during SEM. These factors ultimately contribute to a morphological transformation of the densely packed g-C3N4 to a porous configuration.31,56
Fig. 8 (a) UV-vis spectra and (b) Tauc equation plot of g-C3N4 synthesized at different temperatures. |
To improve the thoroughness of the analysis, photoluminescence (PL) spectra were employed to examine the optical properties of g-C3N4 powders using two distinct excitation light sources with wavelengths at 365 and 405 nm. The PL spectra are illustrated in Fig. 9a and b, for excitation wavelenghts at 365 and 405 nm respectively. The emission peaks observed at distinct wavelengths are attributable to the recombination of electron–hole, which releases light energy equivalent to the band gap energy of the samples of g-C3N4. The energy band gap values obtained through calculation of PL spectrum peaks are presented in Table 1.
Fig. 9 PL spectra of g-C3N4 synthesized at different temperatures by (a) 365 nm (b) 405 nm light source. |
(1) |
Fig. 10 (a) Effect of calcination temperature on the photocatalytic activity of g-C3N4, (b) photocatalytic kinetic constants of g-C3N4. |
The values of (k) for samples CN400, CN450, CN500, CN550 and CN600 were calculated, respectively, 0.0813 min−1, 0.1089 min−1, 0.0517 min−1, 0.0729 min−1, and 0.0270 min−1.
To calculate the position of band structure of g-C3N4 and explore the mechanism of photoreduction of Cr(VI) eqn (2) and (3) were utilized. where ECB and EVB represent the conduction band (CB) and valence band (VB) edge potentials, respectively, Ee (∼4.5 eV) is the free electron energy on the scale of hydrogen, X represents the electronegativity of the semiconductor and Eg is the semiconductor band gap. The value of X for g-C3N4 was calculated as 4.67 eV and by referring eqn (2) and (3) the values of calculated VBs and CBs were shown in Fig. 11.57 Moreover, chromium metal is present in two stable oxidation states, Cr(VI) and Cr(III).58 Given that the colorimetric diphenylcarbazide method exclusively identifies Cr(VI), it is anticipated that the quantity of reduced Cr(VI) has converted to Cr(III).59 Based on the calculated values of CBs and VBs, a possible mechanism of photocatalytic Cr(VI) reduction within the presence of citric acid has been suggested as appeared in Fig. 11. The photogenerated electrons in the CB of g-C3N4 are transferred for the photocatalytic reduction of Cr(VI) to Cr(III), and at the same time the citric acid which acts as a sacrificial agent is trapped by photogenerated holes in the VB of g-C3N4.
(2) |
ECB = EVB − Eg | (3) |
The effect of other process variables on g-C3N4 photocatalytic performance such as pH, citric acid concentration, and recycling ability was investigated under xenon lamp on CN450 and the results are shown in Fig. 12a–c respectively. The effectiveness of the photocatalytic reduction process for Cr(VI) is observed to decrease in a substantial manner with an increase in the pH value as mentioned in Fig. 12a. In addition, when pH is 8 and 11, Cr(VI) cannot be reduced at all. In general, the Cr(VI) species are commonly found in tetrahedral oxo-compounds, specifically in the form of CrO42−, at pH levels greater than 5.0, and while they appear as Cr2O72− or HCrO4− at neutral or acidic pH levels ranging from 2.0 to 5.0. Furthermore, the surface charge of the photocatalyst, attributed to the pH level, constitutes a factor that partially accounts for the observed phenomenon.37,60 The results indicate that an excess quantity of hydrogen ions (H+) is present, namely, a state of acidosis. The phenomenon of reduction from photogenerated electrons is stimulated in an environment with increased acidity, as depicted through eqn (4) and (5):37
Cr2O72− + 14H+ + 6e− → 2Cr3+ + 7H2O | (4) |
HCrO4− + 7H+ +3e− → Cr3+ + 4H2O | (5) |
Fig. 12 (a) Solution pH, (b) citric acid concentration, (c) recycling effects on CN450 photoreduction of Cr(VI) process under xenon lamp and (d) XRD patterns of CN450 before and after photocatalysis. |
In alkaline conditions, electrostatic repulsion between g-C3N4 and Cr(VI) impeded the interaction with photogenerated electrons, resulting in a decrease in the Cr(VI) removal rate by means of eqn (6):37
CrO42− + 4H2O + 3e− → Cr(OH)3 + 5OH− | (6) |
According to active species trapping experiments especially, tert-butyl alcohol, 2,2,6,6-tetramethylpiperidine-1-oxyl, and methanol scavengers, the efficacy of Cr(VI) removal in photocatalytic reduction reactions mediated by g-C3N4 can be enhanced through the augmentation of organic acids acting as hole-scavenging agents. Photoreduction is the mechanism through which Cr(VI) is reduced in water, with the electrons produced in the CB through photon absorption playing a crucial role in the process. The catalytic process of water oxidation leading to the creation of molecular oxygen is primarily driven by the photogenerated holes found in the valence band. As water oxidation is a complex process that determines the rate and it involves a four-electron transfer reaction. Thus, to attain optimal reduction of Cr(VI) while separating electron–hole pairs efficiently, it is necessary to use a hole scavenger. Therefore, the augmentation of the chromium reduction rate as illustrated in Fig. 12b can be rationalized by the amplification of the citric acid concentration.61–63 It should be noted, citric acid monohydrate without any semiconductor can provide Cr(VI) photoreduction under 400 W metal halide lamp as a light source, therefore should be aware about the role of citric acid in Cr(VI) photoreduction. However, it should be mentioned the best performance of citric acid monohydrate Cr(VI) photoreduction observed at higher concentration under more than 300 W metal halide and high-pressure mercury lamps.64
Fig. 12c exhibits the recuperation rate of the CN450 photocatalyst subsequent to each cycle of the photocatalytic procedure for the purpose of Cr(VI) reduction. Notwithstanding a decrease in the photocatalyst quantity during successive rounds, the fourth round demonstrated considerable efficacy in reducing the concentration of chromium to above 98% of its initial level. Additionally, XRD analysis was conducted following four cycles of photoreduction, as illustrated in Fig. 12d. The CN450 material exhibited successful reutilization, showcasing an almost stable photocatalytic performance.
Photocatalytic materials encounter another challenge in their activation by light, as it hinges upon the spectral composition of the incident light and the bandgap energy of the photocatalyst, necessitating optimal alignment between the two. The use of solar radiation has been widely recognized as a highly advantageous approach to activating the photocatalyst, owing to its environmentally friendly nature. Consequently, due to the comparable and full range of the visible spectrum emitted by the xenon lamp, it has been frequently utilized at high power of intensity in numerous photocatalytic research. In contrast, scholars have investigated the viability of visible LED as source. This approach stems from the fact that the intensity of sunlight is contingent upon the geographical position and time of day, however, the conversion of electrical energy into light via xenon lamps leads to a notable production of heat, the efficacy of LED lamps has also undergone comprehensive examination. Such an investigation is elucidated in Fig. 13. As hypothesized, the efficiency of LED lamps is observed to increase in proportion to the reduction of their radiation wavelengths. The present findings indicate a heightened photocatalytic efficiency in the 400 nm LED light source, which exhibits a lower power consumption compared to its xenon-based counterpart.
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