Ruixiao Maab,
Liyan Xieb,
Yixuan Huanga,
Kangji Zhuoa,
Juan Xua and
Yanhui Zhang*ab
aCollege of Chemistry, Chemical Engineering and Environment, Fujian Province Key Laboratory of Morden Analytical Science and Separation Technology, Minnan Normal University, Zhangzhou, 363000, P. R. China. E-mail: zhangyh@mnnu.edu.cn; Tel: +86 596 2591445
bFujian Province Key Laboratory of Ecology-Toxicological Effect & Control for Emerging Contaminants, Putian University, Putian, 351100, P. R. China
First published on 9th August 2021
At room temperature, a facile approach has been utilized for preparing novel CdS–attapulgite (CdS–ATP) composites and the composites were applied in photocatalytic reduction of p-nitrophenol and Cr(VI). The effect of ATP on the photocatalytic activity of the CdS–ATP composites were studied by controlling the mass ratio of attapulgite. The results showed that the CdS–20%ATP composite has an excellent photocatalytic activity. In order to figure out the key to improve the photocatalytic efficiency, the prepared composites were characterized by Brunauer–Emmett–Teller (BET) specific surface area, UV-vis diffuse reflectance spectroscopy (DRS) and electrochemical impedance spectroscopy (EIS). The superior photocatalytic performance of the CdS–20%ATP composite can be ascribed to the existence of the ATP which can fix the CdS and prevent agglomeration. The interaction between ATP and CdS in the composites facilitates the electron transfer and also promoted their photocatalytic performance. This work provides us with some significant guidance in the development of CdS–ATP composite photocatalysts.
Hence, it is urgent to enrich advanced materials and develop versatile technologies for environmental remediation.3,32,33 As a chalcogenide photocatalyst, CdS has attracted much interest because of its narrow band gap, high light harvesting and excellent catalytic properties.34–36 However, the limitations of the high recombination rate of photogenerated electron–hole pairs, photocorrosion problems, and easy agglomeration of CdS hinder its further application in photocatalysis.34,37–39 Therefore, many efforts have been made to optimize the properties of CdS such as the materials hybridization and element doping.35,40,41
Natural attapulgite (ATP) may be used as a perfect support material to hybridize with CdS because of the abundant reserves, attractive price, and special structure. And the ideal formula of the ATP is Al2Mg2Si8O20(OH)2(OH2)4·4H2O. The adsorption, carrier and catalytic properties of ATP make it a promising catalyst in sewage disposal.42–44 In the CdS–ATP composites, ATP may not only play a role in fixing and avoiding agglomeration, but also can reduce light corrosion and improve light tolerance. In addition, as an ideal photocatalytic carrier material, ATP can also provide many microreaction sites for photocatalytic reaction.45,46 Furthermore, the mesopores of ATP also could play the role of facilitating the mass transport in CdS–ATP composites, which may improve the photocatalytic performance in reduction reaction.47,48 If CdS–ATP composites could be successfully compounded, the limitations of CdS can be overcome, making it more targeted in the application of photocatalysis. However, in the photocatalytic treatment of sewage, there is no research on ATP and CdS–ATP composites as photocatalysts. Thus, the application of ATP and CdS–ATP composites in photocatalysis needs to be pioneered and further explored.
Herein, the CdS–ATP composites are used for the photocatalytic reduction of p-NP and Cr(VI), which lays a foundation for the further development of CdS–ATP composites in photocatalysis. The effects of photocatalytic reduction efficiency were investigated by adjusting the mass ratio of the ATP. It was found that the photocatalytic efficiency of CdS–20%ATP composite has the most excellent efficiency under the premise of many microreaction sites that are provided by ATP. It can be attributed to not only the weakened photocorrosion but also the enhanced electron transfer by a series of performance analysis.
The photoreduction efficiency of Cr(VI) was obtained by substituting 40 mg L−1 Cr(VI) for 10 mg L−1 p-NP, 0.05 g of the sample without ammonium formate as a capture agent and the irradiation time interval was shortened from 2 min to 1 min. Plot the changes of C/C0 of Cr(VI) at 373 nm as the ordinate and the irradiation time as the abscissa.
Furthermore, the FT-IR analysis was used to research the chemical composition of the obtained photocatalysts, and the FT-IR spectra of the blank-CdS, ATP, CdS–10%ATP, CdS–20%ATP, and CdS–30%ATP were shown in Fig. 2. In the FT-IR spectrum of blank-CdS, the wavenumber at 674, 1000 and 1380 cm−1 are attribute to the typical absorption of the Cd–S bond.51 In the spectrum of ATP, on characteristic peaks at 800 and 1032 cm−1 can ascribed to the symmetric stretching vibration of Si–O and unsymmetric stretching vibration of Si–O–Si respectively.43 And the broad-band between 3300 and 3500 cm−1 is due to the skeletal vibrations of O–H.43 The major characteristic vibration peaks related to CdS and ATP can be clearly found in the composites, which implying that the structure of CdS remains intact after composited with ATP.
To further identify the chemical composition of the composites, the XPS analysis was applied to compared the different elements in ATP and CdS–20%ATP and the survey spectrum was shown in Fig. 3a. The peaks at binding energies about 405.5 eV and 412.2 eV could match well with the peaks of Cd 3d and the peaks about 175.1 eV could linked to S 2p in Fig. 3b and c.35 In addition, the other detailed elements spectrum of CdS–20%ATP and ATP by XPS analysis were displayed in Fig. S1 (in the ESI†). In the spectrum of Mg 1s, Al 2p, Si 2p and O 1s Fig. S1,† the binding energy was slightly increased after compounding with CdS. Especially, the peaks of Al 2p has a peak separation, this may be due to the effect of CdS on the valence of Al in ATP. All the above phenomenon indirectly also proves that the CdS anchored on ATP surface successfully.
The morphologies of the photocatalysts were studied by SEM and TEM analysis. From Fig. 4a, it can be clearly seen that the rod-shaped structural of ATP, which is consistent with previous reports.52 The as-prepared blank-CdS were aggregated and the size of CdS nanoparticles is around 15 nm as depicted in Fig. 4b. It can be obviously seen that CdS nanoparticles successfully anchored on the surface of ATP support in CdS–20%ATP composite, as depicted in Fig. 4c and d. In addition, the TEM of CdS–20%ATP composite, shown in Fig. 5, further shows us the internal information of the CdS–20%ATP composite. In Fig. 5a, it can be seen that CdS has wrapped the ATP nanorods. The lattice fringes of CdS can be clearly seen in the Fig. 5b, and the spacing of the lattice fringe is 0.336 nm, which could be assigned to the (111) plane of CdS. In addition, the main elements of composite also can be detected from the EDS of CdS–20%ATP in Fig. 5c, and the main elements all be probed. There are three clear diffraction ring in the SAED of CdS–20%ATP, indicates the CdS crystallize well, and this also could be matched with the XRD patterns of CdS–20%ATP. From this results, we can extrapolate that the CdS–ATP composites was successfully prepared.
The photocatalytic activity of CdS–ATP composites were investigated via reduction of p-NP. Fig. 6 demonstrates reduction ratio of p-NP when ammonium formate was used as sacrificial reagents under ambient conditions in water, where C0 was the concentration of p-NP after adsorption for 40 min in the dark and C was the concentration of p-NP after irradiation.
Fig. 6 Photoreduction efficiency with 5% error bars of p-nitrophenol under simulated solar light irradiation for 10 min at room temperature. |
As shown in Fig. 6, the concentrations of p-NP almost has no change when ATP is used as the photocatalyst, indicating that the ATP has no photocatalytic activity in photocatalytic reduction of p-NP. The blank-CdS exhibits a lower photocatalytic activity owing to the high recombination rate of photogenerated charge carriers.37 Obviously, the CdS–20%ATP composites exhibits the optimal weight percent and has the highest reduction efficiency among the above samples in 10 min, giving a 2.6 times higher rate of p-NP reduction than blank-CdS. Indeed, we have also used the high performance liquid chromatograph (HPLC) to quantify the distribution of reactant and product, which confirms that the product is primarily dominated by p-AP with a high selectivity.
The blank experiment without ammonium formate was conducted in order to figure out the effect of ammonium formate during the photocatalytic reduction of p-NP. The UV-vis absorption characteristics of p-NP over blank-CdS and CdS–20%ATP was shown Fig. S2 (in the ESI†). As shown in Fig. S2,† it can be found that in the absence of ammonium formate, the absorbance of p-NP changes little, which indicates that ammonium formate is the key to photocatalytic reduction of p-NP.
The photocatalytic reduction of Cr(VI) has also been studied. Fig. 7a displays the photocatalytic efficiency of Cr(VI) with the samples of blank-CdS, ATP and different mass rations of CdS–ATP composites as photocatalysts. After adding the chromophoric reagent, the UV-Vis absorption spectrum indicates that the reduction product was mainly Cr(III) when the content of Cr(VI) decreases. Moreover, the pseudo-first-order relationship was revealed in Fig. 7b. The order of the kinetic rate constants are as follows: CdS–20%ATP (0.4467 min−1) > CdS–10%ATP (0.3177 min−1) > CdS–30%ATP (0.2435 min−1) > blank-CdS (0.1903 min−1) > ATP (0.0040 min−1). As the mass ratio of ATP increases, the photocatalytic activities of CdS–ATP composites increase first, achieve a peak value at CdS–20%ATP, and then decrease. Which is consistent with the reduction of p-NP. The possible reasons are put forward as follows: under simulated solar light irradiation, with a low mass ratio (CdS–10%ATP), the photocatalytic activity of the CdS is improved by being mixed with ATP, which is beneficial to boost the light absorption in the visible and ultraviolet regions. Then, the photocatalytic activity of CdS–ATP composites can be enhanced with the increase in the ATP amount. After the maximum, the photocatalytic activity of CdS–ATP composites decreases with the increase of ATP (CdS–30%ATP). This could be due to excessive ATP that covers the active sites of CdS, which hinders the light absorption and electron transfer, thus, in turn inhibits the photocatalytic activity.
Fig. 7 Photocatalytic reduction of Cr(VI) under simulated solar light irradiation with 5% error bars (a) and the apparent rate constant (ka) (b) in 5 min at room temperature. |
In order to explore the effect of pH on the reaction, we adjusted the pH to 3 for photocatalytic experiment under the same conditions. The UV-vis absorption spectrum of Cr(VI) was shown in Fig. S3 (in the ESI†). As the pictures depicted, the characteristic absorption peak of Cr(VI) at 373 nm disappeared. That reason may be that the Cr(VI) could convert to Cr(III) easily according to the formula: Cr2O72− + H+ → 2Cr3+ + H2O.53 When reduction of p-NP, the conversion was hindered when pH = 3 from Fig. S4 (in the ESI†). Because the acidic condition is not conducive to the deprotonation of p-NP.19
UV-vis DRS analysis was conducted in order to investigate the optical properties of all the samples. As illustrated in Fig. 8, in ultraviolet region all samples have strong absorption. The absorption edge of ATP is about 400 nm, means a weaker absorption in visible region. However, the absorption edge of blank-CdS is about 600 nm, suggesting an excellent light absorption in visible region. Compared with blank-CdS, the absorption edge of CdS–ATP composites have a slight blue shift, but it has a insignificant effect on the light absorption capacity. That is to say, the light absorption is not enhanced in CdS–ATP composites, thus, the light harvesting efficiency is not the main factor of the photocatalytic activity.
The N2 adsorption–desorption experiments were carried out to get the Brunauer–Emmett–Teller (BET) specific surface area and the porous structure of ATP, blank-CdS and CdS–20%ATP. According to the IUPAC classification, as seen from Fig. S5 (in the ESI†), the N2 adsorption–desorption isotherms of the ATP shows a type III adsorption–desorption isotherm with a H3 hysteresis loop indicating the presence of mesopores.54 The blank-CdS and CdS–20%ATP composites both exhibit a type V adsorption–desorption isotherm which is similar to the type III. As depicted in Table 1, the surface area of CdS–20%ATP decreased little compared with the blank-CdS. As seen from Fig. S6 (in the ESI†), the normalized Ka/SBET of all the photocatalysts, the CdS–20%ATP composites shows the largest Ka per m2, indicating the 20% of ATP is the optimal ratio in composites. That may be the effect of mesopores in CdS–ATP composites which could promote the mass transport rather than the specific surface area.47,48 That may be why the CdS–20%ATP composites has the best catalytic efficiency though the surface area changes little.
Sample | SBET (m2 g−1) | Pore size (nm) |
---|---|---|
ATP | 105 | 6.8 |
Blank-CdS | 128 | 5.7 |
CdS–10%ATP | 112 | 9.7 |
CdS–20%ATP | 127 | 12.4 |
CdS–30%ATP | 138 | 11.6 |
In order to study the carrier separation of the photocatalyst, the photoelectrochemical properties of ATP, blank-CdS and CdS–20%ATP were evaluated by electrochemical impedance spectroscopy (EIS). It is worth noting that, compared with other samples, the introduction of ATP leads to distinctly decrease in the arc for CdS–20%ATP as seen in Fig. 9. This is favorable evidence that, on CdS–20%ATP, carrier transfer is more effective than other samples. Therefore, it is clear that CdS with rod-shaped crystal aggregates of ATP can promote the interfacial electron transport more efficiently than blank-CdS and ATP. And that's why CdS–20%ATP exhibits a higher efficiency in reduction of p-NP and Cr(VI) than blank-CdS.
To evaluate whether CdS–20%ATP was reusable as photocatalysts, the recycled experiments for photoreduction of p-NP has been performed, and the results are shown in Fig. 10. During four successive cycles, there is no obvious photocatalytic activity loss in reduction of p-NP under the simulated sunlight irradiation, suggesting that CdS–20%ATP composites have an excellent stability for the photoreduction. In addition, we also investigated the crystal structure of XRD analysis of CdS–20%ATP composites after four successive cycles in reduction of Cr(VI), as depicted in Fig. S7 (in the ESI†). From the XRD pattern, there is no obviously change in the crystal structure of CdS–20%ATP composites after four cycles, which also indicating that the CdS–20%ATP is stable and light-resistant.
Fig. 10 Recycle testing of the photoreduction efficiency of CdS–20%ATP of p-NP under simulated solar light irradiation in water. |
When the simulated solar light starts to irradiate, the electrons in the valence band of CdS are excited to transition to its conduction band and convert into photogenerated electrons.
The photogenerated holes remain in the valence band, correspondingly. Furthermore, due to the lower resistance of charge transfer in CdS–20%ATP composites, the lifetime of photogenerated carriers is effectively extended, which is very beneficial to photocatalytic reduction. The existence of mesopores in CdS–20%ATP composites also could accelerate the mass transport during the reaction. In the reduction of p-NP, the photogenerated holes trapped by ammonium formate, and the photogenerated electrons worked on p-NP to turn into p-AP. In this reaction, the ammonium formate is pivotal for triggering the photoreduction because without the hole sacrificial agent the reaction is difficult to start. As for Cr(VI), the experiment can be carried out without sacrificing agent. Similar to typical photocatalytic reactions, the photogenerated electrons captured by Cr(VI), and then reduced into Cr(III).
Based on the above experiments and analysis, the probable photocatalytic reduction mechanism for CdS–20% ATP is proposed, as shown in Fig. 11 (Take reduction of p-NP as the example).
Footnote |
† Electronic supplementary information (ESI) available: Mg 1s, Al 2p, Si 2p and O 1s XPS spectra of CdS–20%ATP and ATP; The UV-visible absorption spectra of p-NP without ammonium formate by blank-CdS and CdS–20%ATP; the UV-visible absorption spectra of Cr(VI) when pH = 3 with CdS–20%ATP as catalyst; the photocatalytic reduction of p-NP when pH = 3 with CdS–20%ATP; N2 adsorption–desorption isotherms of the ATP, blank-CdS, and CdS–20%ATP; the image of normalized Ka/SBET of the blank-CdS, CdS–10%ATP, CdS–20%ATP and CdS–30%ATP; XRD patterns of CdS–20%ATP 4th run. See DOI: 10.1039/d1ra04530j |
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