3.1 Mechanism for biofabrication of SnO2 NPs
The mechanism for the fabrication of SnO₂ NPs is illustrated in figure 2. The leaves extract dissolved in water is thoroughly mixed with the dissociated tin cations. The hydroxyl groups attached to the aromatic compounds provide active sites, making them prone to form tetravalent bonds. Concurrently, water molecules interact with this tetravalent complex, generating hydrogen bonds. Additionally, the presence of organic components stabilizes the intermediate product and prevents aggregation. Finally, calcination is performed as the last step, decomposing the organic residues and yielding SnO₂ NPs [34][35].
For the leaves utilized in this study, the most likely phytochemical compounds involved in the reaction process are identified as flavonoids. These compounds are shown in figure 3. These flavonoid compounds are known as quercetin 3-O-β-D-glucopyranoside (L-epicatechin) and 2-(3,4-dihydroxyphenyl)-3,4-dihydro-2H-chromene-3,5,7-triol (catechin) from M. citrifolia [36] and P. amaryllifolius [37], respectively. Based on the proposed mechanism, it is suggested that the hydroxyl groups located at the para- and meta-positions of the aromatic rings make these compounds susceptible to and compatible with the reaction, given their significant presence in the leaves. Another aspect supporting this proposal, besides the suggested mechanism, is the well-documented evidence in prior literature that flavonoids possess strong chelating abilities, especially in the adsorption of metal ions [38][39][40][41]. Consequently, this characteristic facilitates the formation of coordination bonds between the tin cations and hydroxyl molecules, enhancing the overall efficacy of the process. By examining the proposed molecular structure, comparisons were made to previous research on the biosynthesis of SnO₂ NPs. It was found that nearly all the proposed phytochemical compounds were polyphenolic flavonoids or compounds heavily bonded with hydroxyl groups [42].
3.2 Fourier transform infrared (FTIR) analysis
The absorption bands of the synthesized SnO2 NPs from M. citrifolia and P. amaryllifolius employing various extract to precursor salt ratios are visible in the infrared spectra shown in figures 4. The purpose of this investigation was to investigate the existence of relevant functional groups for the SnO2 synthesis. The results indicate that there are two primary sets of absorption peaks present in all examined samples: the stretching vibration of Sn-OH and the anti-symmetry vibration of Sn-O, which are located in the 600 to1000 cm-1 range, respectively [43][44][45].
The findings indicate that Sn-O anti-symmetrical vibration peaks are uniformly distributed in the same area and show almost the same strength throughout the proposed ratio range. On the other hand, the Sn-OH peaks show up regardless of the fluctuation in the applied extract concentration. This may be explained by the competing hydrogen bonding that occurs between the phytochemicals and the OH group of water molecules, which produces distinct capping volumes on the surface of Sn4+ and, in turn, diverse Sn-OH vibrational or stretching patterns. Furthermore, CO2 absorption peaks have been found in the vicinity of 3000 cm-1 [46], which has led to some spectrometer tuning fluctuation about 2200 cm-1. Nevertheless, these peaks are negligible. Overall, it is feasible to produce SnO2 NPs sustainably by using these ratios.
3.3 X-ray diffraction (XRD) analysis
The XRD spectra of the synthesized SnO2 NPs derived from M. citrifolia and P. amaryllifolius are shown in figure 5, using JCPDS card no. 01-077-0452. The collected peaks at 2θ values of 26o, 33o, 37o, 51o, 54o, 57o, 61o, 64o, 65o, 70o, 78o and 83o can be indexed as (110), (10 1), (200), (211), (220), (002), (310), (112), (301), (202), (321) and (222) planes. In addition, high intensity peak attributed from tetragonal shape and crystalline in nature was observed at 26o, 33o and 51o, that belongs to Braggs reflections of (110), (101) and (211) set of lattice plane. The XRD patterns acquired corroborate with the past works of literature [47][48][49]. By using the Scherrer formula, D= kλ/β cos θ, the average nanocrystalline size was calculated based on the plane with the highest atomic density in SnO2 NPs, which is (110) [50]. Regarding this formula, D is particle diameter size, k is Cu Ka (1.54 Å) X-ray wavelength of the X-ray source, β is the full width at half maximum (FWHM), θ is the diffraction angle and k is the unknown shape factor [51].
Given that the most crystalline SnO2 NPs are representative of peak intensity, altitude, and narrowness, 3:1 is the preferred ratio for M. citrifolia for these reasons. The nanoscale dimension of the crystallite was determined to be 29.19 nm using the Scherrer formula. It is thought that the hydroxyl group of phytochemicals participates in Sn4+ reduction during the capping action, which requires less energy to weaken the bonding of the O-H bonds and increases its susceptibility to carrying out the capping action [52]. This process is assumed to reach saturation at a ratio of 3:1, at which point highly dense polyphenolic phytochemicals bind to Sn4+ with steric hindrance, causing uncapped Sn4+ to agglomerate. This increases the likelihood that agglomeration will be prevented, leading to large crystallite size.
For the case of P. amaryllifolius work-based, when the extract ratio was increased, the XRD peaks for the P. amaryllifolius work-based example show dependency. Lower extract concentrations provide XRD peaks that are sharp and intense, giving a preferred ratio of 1:1 results in a crystallite size of 9.02 nm. A comparable phenomenon of a reduction in peak intensity was also noted while employing Citrus aurantifolia [26], Tradescantia spathacea [43], Camellia sinensis [53], Lycopersicon esculentum [54], Tilia cordata [55] whenever the extract's concentration rises. The phytochemicals in the extract are probably what cause this phenomena because they disrupt the SnO2 NPs' crystallinity, which causes a less organized arrangement of atoms on the surface [53]. Another explanation can be related to the synergistic impact of the hydroxyl groups, which allows them to do two tasks whenever possible: they can operate as dispersants because of the C=O bond, as well as a reducing and capping agent. Consequently, the dispersion activity of SnO2 NPs reduces the clumping problem when ratios between 1:1 and 5:1 are used.
Table 1. The crystallite size of SnO2 NPs derived from M. citrifolia and P. amaryllifolius.
Ratio of extract to precursor salt
|
M. citrifolia
|
P. amaryllifolius
|
Crystallite size D (nm)
|
FWHM (oC)
|
Crystallite size D (nm)
|
FWHM (oC)
|
1:1
|
13.25
|
0.67
|
9.02
|
1.03
|
3:1
|
29.19
|
0.25
|
6.92
|
1.31
|
5:1
|
12.32
|
0.75
|
6.10
|
1.50
|
3.4 Field emission scanning electron microscopy (FESEM) and energy dispersive X-ray spectroscopy (EDX) analysis
FESEM and EDX analyses were conducted using SnO2 NPs with a ratio of 3:1 for M. citrifolia-based sample and a ratio of 1:1 for P. amaryllifolius-based sample. Figure 6 demonstrates the morphological images of SnO2 NPs with tinny spherical SnO2 NPs with rigid agglomeration are produced when M. citrifolia extract concentration is applied in an equivalent proportion to a precursor salt solution. This is consistent with earlier research on biosynthesized SnO2 NPs, which showed morphological results that were either spherical or quasi/semi-quasi forms [56][57][58]. The homogeneity of the nanospheres, which lowers agglomeration, is thought to be caused by the hydroxylated flavonoid contained in the leaf extract consistently having stabilizing activity [59]. When compared to the two succeeding samples, the spherical morphology shown in SnO2 NPs derived from P. amaryllifolius shows that incredibly small nanoparticles was produced. These nanoparticles appear as a spherical sponge-like shape upon examination. It may be deduced that increased electrostatic contacts are the outcome of the capping action carried out on the Sn4+ surface by the relevant phytochemicals. Subsequently, it causes a progressive adjustment of thermodynamics, which results in a marginal variation in the orientations of atomic groupings. This ocassion is in line to the author's view in Tilia cordata work-based, where the author suggests that limited nucleation of nanoparticles due to significant phytochemical interference could lead to a variety of forms in nanoparticles [55]. Since tiny nanoparticles are present in SnO2 NPs, it is doubtful that the nanoscale measurements for both samples will be obtained.
The atomic percentages of Sn and O in SnO2 NPs derived from M. citrifolia are 34.39% and 65.61%, respectively as shown in table 2. Meanwhile,the atomic percentages of Sn and O for P. amaryllifolius are 69.31% and 30.69%, respectively. The composition of Sn and O levels are within an acceptable range and are in line with earlier research, confirming the elements purity [60][61].
Table 2. The atomic percentages of SnO2 NPs.
Work-based
|
Ratio of extract to precursor salt
|
Atomic (%)
|
Sn
|
O
|
M. citrifolia
|
3:1
|
34.39
|
65.61
|
P. amaryllifolius
|
1:1
|
30.69
|
69.31
|
3.5 High Resolution transmission electron microscopy (HRTEM) and selected area diffraction (SAED) analysis
The HRTEM reaults reveal that the sample consists of well-crystallized nanoparticles with varying particle sizes. The consists visibility of lattice fringes across different regions indicates high crystaallinity throughout the sample. This might be due to different synthesis conditions of post-synthesis treatments. Figure 7a and b depict aggregated nanoparticles with a roughly spherical shape for M. citrifolia experimental, while significant spherical shape with a highly polycrystalline structure and some minor agglomerates for P. amaryllifolius work-based. These morphological findings are consistent with FESEM images, which show spherical formations of SnO2 NPs derived from P. amaryllifolius and not to M. citrifolia work-based. The particle size distribution appears to vary within different regions of the sample, as indicated by the inset histograms in Figure 4a and 4c. The mean particle sizes give values of 3.24 nm for M. citrifolia and to 7.63 nm for P. amaryllifolius. This finding is believed within the optimal range for producing finely tuned nanoparticles for photocatalytic testing.
The interplanar distances for all samples shown in figure 7b and d are comparable to those obtained from XRD analysis, as tabulated in Table 3. Notably, P. amaryllifolius work-based obtained values of d indicate a correlation for the (101) plane, unlike the (110) planes obtained from M. citrifolia experimental or other reports. Following the principle of lowest energy, active sites of the nuclei might encourage nanoparticles to grow along the most stable crystal face, indicating that the preferential growth lattice plane is (101) rather than the conventional (110) plane. Consequently, the surface energy in various crystallographic orientations follows to the order (101) > (110) [62]. Additionally, the SAED spectra exhibits multiple rings consistent with XRD diffraction peaks (Figure 7e and f). As expected, the highly crystalline nature of SnO2 NPs provides prominent diffraction rings corresponding to reflections (110), (101), (200) and (211) [54][63]. The pattern displays distinct diffraction spots arranged in rings, which is characteristic of polycrystalline materials. The presence of these indexed planes indicates the materials’s crystallographic orientations and confirm its prolycrystalline nature. The pattern suggest the presence of multiple crystallinedomains oriented in different directions, contributing to the ring-like appearance of the diffraction spots. The distinct diffraction spots in the SAED patterns confirm the high crystallinity of the sample. The sharpness and clarity of these spots indicate well-ordered crystaalline regions within the material. The indexed planes correspond to known crystallographic planes of specific phases, providing insights into the phase composition of the sample. The consistent indentification of (110), (101), (200) and (211) planes suggests a common phase throughout the sample. The ring-like arrangement of diffraction spots in both patterns is typical of polycrystalline samples. This indicates that the sample consists of numerous small crystallites with random orientations. The SAED results are conssistent with the HRTEM findings, where lattice fringes corresponding to specific planes were observed. This corelations strengthens the overall analysis, confirming the materials crystalinity and phase purity.
Table 3. The comparable d values of SnO2 NPs obtained via TEM and XRD
Work-based
|
TEM d value (Å)
|
XRD d value (Å)
|
Plane hkl
|
M. citrifolia
|
3.25
|
3.28
|
(110)
|
P. amaryllifolius
|
2.55
|
2.36
|
(101)
|
3.5 UV-Vis Diffuse Reflectance (UV-DRS) analysis
The reflectance characteristics of SnO2 NPs derived from M. citrifolia and P. amaryllifolius using a variation of extract to precursor ratio are illustrated in Figure 8 (left). The reflectance edges for all samples of SnO2 NPs fall within the visible region. SnO2 NPs obtained from M. citrifolia demonstrate a reflectance edge at 511 nm with a corresponding reflection of 51%, while from the result of P. amaryllifolius experimental, the reflectance values were recorded as 59% and fall at 527 nm, accordingly. The reflectance values are employed to compute energy band gap, using the Kubelka-Munk formula F(R) = (1-R)2/ 2R = k/s, where F(R) is the Kubelka-Munk functions, and k, s are the K-M scattering and absorption coefficients, respectively [64]. The energy band gap spectrum is constructed by plotting the square of the Kubelka-Munk function against energy and extending the linear portion of the curve, as illustrated in the depicted in figure 8 (right).
The energy band gaps 3.70 and 3.51 eV are observed for M. citrifolia and P. amaryllifolius-based, respectively. By having these values, it is indicated that they require low energy for photoactivation and the application of the photocatalyst to the visible region is said to be compatible [65]. This finding is also very much in agreement with the optimal ratio suggested by the sharpness and intense peak in XRD analysis.
3.6 Analysis of Zeta Potential
In this study, the ZP values for SnO2 NPs derived from M. citrifolia and P. amaryllifolius were found to be -51.1 and -30.7 mV, respectively. These values indicate good electrical stability and suggest a well-dispersed colloidal system with minimal agglomeration [66].
Table 4. Zeta potential of SnO2 NPs
Work-based
|
ZP (mV)
|
M. citrifolia
|
-51.1
|
P. amaryllifolius
|
-30.7
|
3.6 Photocatalytic activities
The photocatalytic activity of the SnO₂ NPs was evaluated through experiments using different catalytic loadings and pH levels, with measurements taken at 10-minute intervals. All samples were stirred in the dark for 30 minutes prior to irradiation to achieve an adsorption-desorption equilibrium [67]. The following formula is used to compute the percentage of dye degradation, where C0 is the dye's initial concentration prior to illumination and Ct is its concentration following time t [68].
Degradation % = (C0 - Ct) /C0 x 100
The results are shown in figure 9. It was found that the degradation of methylene blue (MB) using SnO₂ nanoparticles from both photocatalysts exhibited a turbidity effect. The highest degradation rates were 97% and 80% with a 200 mg loading (Fig. 9a and 9b). It is presumed that the generation of O₂-• and OH• radicals were diminished, leading to a decrease in degradation efficiency, and that catalyst particle accumulation occurs when the catalyst amount exceeds the optimal level. The higher photodegradation performance of SnO₂ NPs derived from M. citrifolia may be due to their smaller particle size, as indicated by HRTEM results, which show a nanoscale size of 3.24 nm compared to 7.63 nm for P. amaryllifolius-derived SnO₂. The smaller particle size may facilitate easier agglomeration, thereby increasing the turbidity of the solution and making part of the catalyst surface unavailable for photon absorption [69]. A previous study described a similar scenario during the removal of rose bengal (RB) under UV irradiation, where degradation initially increased due to enhanced active sites and particle density but later encountered interference from agglomeration with increased photocatalyst loading [70].
The photocatalytic reaction was proceeded using the optimal catalyst loading of 200 mg for SnO₂ NPs derived from M. citrifolia and P. amaryllifolius under three different pH levels: 3, 7, and 11. During the reaction setup, the pH was carefully adjusted to 3 using 0.1 M of HCl and to 11 using 0.1 M of NaOH, added dropwise into the solution. From the results, methylene blue (MB) was optimally photodegraded at rates of 97% and 80% using SnO₂ NPs derived from M. citrifolia and P. amaryllifolius, respectively, as illustrated in figures 9c and d. The photodegradation of MB with all samples of SnO₂ NPs followed a similar pattern, with the highest degradation observed under neutral conditions (pH 7). This suggests that the breakdown of MB molecules is not favoured by these SnO₂ NPs photocatalysts at lower or higher pH levels. Under acidic conditions, the attraction of MB molecules to the surface of SnO₂ nanoparticles is diminished due to the competitive forces exerted by H⁺ ions, resulting in lower degradation rates. In alkaline conditions, the increased concentration of hydroxyl ions leads to more reactions with holes, generating more OH• radicals. However, this results in the desorption of OH• along with dye molecules on the surface of the SnO₂ NPs, inhibiting MB degradation. Optimal degradation occurs under neutral conditions, where the negatively charged surface of SnO₂ NPs enhances the electrostatic attraction with MB molecules. This increases the photo-oxidation rate with minimal recombination of electron-hole pairs, leading to efficient degradation of MB molecules. This behaviour contrasts with the degradation of rhodamine B by SnO₂ NPs prepared from C. ternatea flowers, which was rapid under both acidic and basic conditions [71]. However, it is consistent with the degradation of methyl orange reported in experiments using C. gigantea, which showed a preference for nearly neutral conditions (pH 6.5) [32].
Figure 10 is a schematic representation of the general photocatalytic degradation process of MB using SnO₂ NPs. Three phases are hypothesized for the degradation process: adsorption (i), oxidative species production (ii) , and final MB molecule breakdown (iii to v) [54][72][73]. SnO2 NPs capacity to draw MB molecules more strongly to their surface is necessary for the adsorption of MB molecules on their surface. Subsequently, the light-induced oxidative species formation in SnO2 produces holes (h+) in the valence band (VB) and electrons (e-) in the conduction band (CB). At this time, photogenerated e- will reside in CB and photogenerated h+ will reside in VB after being sent in the opposite direction. Later, at the surface of SnO2 NPs, e- reacts with dissolved oxygen (O2) to oxidize it and produce superoxide radicals (O2-•), and h+ oxidizes H2O molecules to produce hydroxyl radicals (OH•). These two species break down MB molecules because they are strong oxidizers. Here, S-Cl, N-CH3, CS, CN, and C-O bonds were broken during the degradation process, resulting in fragments of 4-(N,N-dimethyl)-aniline and 3-(dimethylamino)benzenesulfonate. As a result, a series of intermediate products degrade, causing the MB rings to open and smaller organic molecules to form [72]. This process continues until total mineralization is reached, producing the reaction known non-hazardous by-products, H2O and CO2. The transition from blue to colorless is a powerful sign of the SnO2 surface great adsorption capability, which is caused by the MB molecule π-π interactions [74].
The primary oxidative species involved in the photodegradation of MB are identified by radical trapping experiments, referred to as scavenger tests, in order to further elucidate the potential reaction mechanism of MB photodegradation by biosynthesized SnO2 NPs. The purpose of this experiment was to identify the particular reactive species that cause MB degradation. The MB solution containing the optimized SnO2 NPs was supplemented with approximately 1 mL of 2 mM of different scavenger reagents in this study. The optimized photodegradation parameters were then employed in the process. These reagents were isopropanol (IPA) for hydroxyl radicals (OH•), EDTA for photogenerated holes (h+), benzoquinone (BQ) for superoxide radicals (O2-•), and AgNO3 for electrons (e-) [75]. The result shows in figure 11 indicates that AgNO3 inhibits the photocatalytic degradation efficiency of MB by SnO2 NPs produced from both plant sources, meanwhile the kinetic momentum for degradation activity is retained by BQ, EDTA, and IPA. These findings imply that superoxide anion (O2-•), hydroxyl radical (OH•), and photogenerated hole (h+) have a negligible inhibitory effect on the photocatalytic process, however the introduction of electrons (e-) from AgNO3 inhibits the photocatalytic activity. The removal rate of MB dramatically decreased to 55% and 15% for M. citrifolia and P. amaryllifolius experimental, respectively, remarkably with the addition of AgNO3. This suggests that the active species involved in the elimination of MB are e- [76]. EDTA acts as a scavenger for h+ to prevent the recombination of electrons and holes, but no discernible inhibition was seen [77]. Moreover, it is discovered that O2-• from BQ is less successful in preventing the breakdown of O2. Furthermore, O2-• from BQ is found to be less effective in inhibiting the dissolution of O2 [78]. This finding contradicts previous scavenging experiments using SnO2 NPs from T. cordifolia [77] , P. pinnata [19] and C. ternatea [71], which indicated that the main reactive species are OH• from IPA. The scavenging activity was explained by the radical ability to be trapped by surface and photonic contacts, which in turn decreased the production of further oxidation.
Because it aligns with practicality and cost considerations while performing dye-polluted water, photocatalyst stability is important for practical applications [79][80]. As a result, five repetitions of the photocatalytic evaluation were carried out utilizing optimized SnO2 NPs that were extracted from the methylene blue (MB) dye following the ideal degradation condition. Water, methanol, and acetone were used to thoroughly wash the SnO2 NPs until all traces of blue staining were completely removed from their surface. Before being utilized again for more catalytic cycles, the recovered SnO2 NPs were dried in a drying cabinet. The weight of the SnO2 NPs catalyst was changed in relation to the MB volume for every cycle.
After achieving a 97% efficiency in the first dye degradation cycle, the degradation efficiencies of SnO2 NPs obtained from M. citrifolia decreased gradually to 75% and 74% in the second and third cycles, 52% in the fourth cycle, and 29% in the fifth cycle (Figure 12a). In contrast, the first degradation efficiency of 80% in the experimental setting with P. amaryllifolius dropped to 46% in the second cycle as shown in figure 12b. This was followed by a progressive reduction, with degradation rates stabilizing at roughly 46%, 43%, 40%, and 38%, respectively, by the fifth cycle. The observed drop can be attributed to the ultimate decline in activity and reaction rate, indicating a limitation in the photocatalyst efficiency [81]. For all samples, the SnO2 NPs photocatalyst's degradation efficiency generally drops over the course of five consecutive cycles. Agglomeration of SnO2 NPs may have caused this decrease by lowering the overall volume of specific surface area [82]. Nevertheless, in completing the photodegradation of MB, the SnO2 NPs photocatalyst demonstrates commendable recyclability. The fascinating findings demonstrate that the SnO2 NPs photocatalyst could be recycled up to five times with only a slight decline in degrading efficiency. This confirms that the SnO2 NPs photocatalyst exhibits remarkable stability and reusability, making it a useful catalyst for the ecologically benign degradation of dyes and organic contaminants.