Muhammad
Ikram
*a,
Fahad
Rasheed
b,
Ali
Haider
c,
Sadia
Naz
d,
Anwar
Ul-Hamid
*e,
Anum
Shahzadi
f,
Junaid
Haider
d,
Iram
Shahzadi
g,
Shaukat
Hayat
b and
Salamat
Ali
b
aSolar Cell Applications Research Lab, Department of Physics, Government College University Lahore, Lahore, 54000, Punjab, Pakistan. E-mail: dr.muhammadikram@gcu.edu.pk
bDepartment of Physics, Riphah Institute of Computing and Applied Sciences (RICAS), Riphah International University, 14 Ali Road, Lahore, Pakistan
cDepartment of Clinical Sciences, Faculty of Veterinary and Animal Sciences, Muhammad Nawaz Shareef University of Agriculture, Multan, 6000, Pakistan
dTianjin Institute of Industrial Biotechnology, Chinese Academy of Sciences, Tianjin 300308, China
eCore Research Facilities, King Fahd University of Petroleum & Minerals, Dhahran, 31261, Saudi Arabia. E-mail: anwar@kfupm.edu.sa
fFaculty of Pharmacy, The University of Lahore, Lahore, Pakistan
gPunjab University College of Pharmacy, University of the Punjab, 54000, Pakistan
First published on 27th July 2022
Graphene oxide (GO) and cellulose nanocrystal (CNC)-doped TiO2 quantum dots (QDs) were effectively synthesized by employing the co-precipitation method for the degradation of dyes and antimicrobial applications. A series of characterizations, i.e., XRD, FTIR, UV-visible spectroscopy, EDS, FE-SEM, and HR-TEM, was used to characterize the prepared samples. A reduction in PL intensity was observed, while the band gap energy (Eg) decreased from 3.22 to 2.96 eV upon the incorporation of GO/CNC in TiO2. In the Raman spectra, the D and G bands were detected, indicating the presence of graphene oxide in the composites. Upon doping, the crystallinity of TiO2 increased. HR-TEM was employed to estimate the interlayer d-spacing of the nanocomposites, which matched well with the XRD data. The photocatalytic potential of the prepared samples was tested against methylene blue, methylene violet, and ciprofloxacin (MB:MV:CF) when exposed to visible light for a certain period. The antibacterial activity of GO/CNC/TiO2 QDs against Staphylococcus aureus (S. aureus) and Escherichia coli (E. coli) bacteria in vitro was tested to determine their potential for medicinal applications. The molecular docking investigations of CNC-TiO2 and GO/CNC-doped TiO2 against DNA gyrase and FabI from E. coli and S. aureus were found to be consistent with the results of the in vitro bactericidal activity test. We believe that the prepared nanocomposites will be highly efficient for wastewater treatment and antimicrobial activities.
Generally, the factors affecting the photocatalytic activity of TiO2 include its energy band gap, photogenerated excitons, lifetime, and large surface area.1–3 Large band gap values (3.0 and 3.2 eV) and reduced quantum efficiency impair the photocatalytic performance of rutile and anatase TiO2 structures.4 However, achieving a large band gap is a significant challenge. Accordingly, doping and dye-sensitization are the most common ways to enhance its optical response in the visible light region. In general, energy intensive methods are utilized for doping other elements in TiO2, such as hydrothermal treatment and high-temperature annealing. Dye-sensitization necessitates that dye molecules, when irradiated, transport photoexcited electrons to the conduction band (CB) of TiO2. Furthermore, the dye molecules in water environment must be very stable. However, upon dye sensitization, charge transfer in visible light-induced photocatalysis occurs from the surface of the complex rather than the absorption of visible light through self-sensing. Consequently, many chemicals not absorb visible light, making them plausible sensitization candidates.5–8
Different approaches have been suggested in the last decade to overcome the above-mentioned disadvantage of TiO2 including doping with non-metals and metals, sensitizing through dyes and compositing with materials such as carbon nanotubes (CNTs) and graphene. Among them, due to the high specific surface area and electrical conductivity of graphene, when it is doped in TiO2, it accepts and transmits photo-generated electrons from TiO2, enhancing the charge separation.9–12 In this case, the structure of TiO2 would considerably improve the photocatalytic activity under visible light in the presence of another element, therefore adjusting its higher Eg (UV area) to a lower Eg (visible light region).
Another material used for this investigation is cellulose nanocrystal (CNC), which possesses exceptional mechanical strength, a wide surface area, and negatively charged sulfuric groups (besides hydroxyl groups being present on the surface of CNC).5 Because of its enhanced crystallinity and good interfacial interaction, CNC exhibits potential to significantly increase the mechanical performance, thermal stability, barrier characteristics, and optical strength of composites. Various studies confirmed that the homogeneous mixing of CNC and GO results in their good integration through hydrogen bonding and intermolecular interactions, and the presence of abundant oxygen-containing groups in GO-CNC composites make them very hydrophilic and allow them to be easily dispersed in water and other organic solvents.13–15 Similarly, Lv et al. concluded that the hydrogen bonding interaction between the hydroxyl groups of CNC and GO sheets facilitates their excellent hydrophilicity by the efficient dispersion of GO sheets and also improves the negative zeta-potential of the resulting composite.16 CNC can also be exploited to stabilize nanoparticles with unique functionality for specific applications. Furthermore, CNC has recently been explored for application in drug delivery systems due to its biocompatibility, biodegradability, and absence of cytotoxicity.17,18
It is well established that most bacterial cell walls (E. coli and S. aureus) are negatively charged. Indeed, certain substances (quaternary ammonium compounds, molecules, and polymers) can electrostatically interface with the negatively charged bacterial surface, and therefore induce membrane rupture and eventual posterior death. The presence of hydroxyl groups makes it ideal for active ingredients and water molecules to connect in a hydrogen-bonded network, encouraging these chemicals to bind, and subsequently transfer to the skin.19 Recently, nanoparticles (NPs) have been employed as an alternative strategy for the treatment of infections caused by resistant microorganisms owing to their unique physical and chemical characteristics. Considering the therapeutic potential of NPs and nanocomposite systems, which promise potentially wide applications in biomedical sciences, a clear understanding of their mechanism of action is desirable. Given that enzymes represent key virulence factors responsible for various microbial infections, inhibiting their activity will aid in finding treatments for diseases. NPs tend to inhibit the activity of various enzymes essential for bacterial growth by binding inside their active pocket.20,21 Accordingly, targeting enzymes belonging to key biosynthetic pathways represents an effective strategy to identify the effects of these NPs on their activity and to explore the potential of these NPs as possible inhibitors and antibacterial agents. The use of computational techniques such as molecular docking studies for a clear understanding of the underlying mechanism of the bactericidal activity of nanocomposite systems is well documented.22,23 Based on this background, we believe that use of GO/CNC co-doped TiO2 QDs as a photocatalyst in combination with ultrasound irradiation to treat wastewater is promising. Further, to the best of our knowledge, the fabrication of GO/CNC-doped TiO2 QDs and their antimicrobial activity and use for the degradation of organic contaminants have not been reported to date.
This study aimed to co-precipitate GO/CNC-doped TiO2 nanostructures and test their photocatalytic and antibacterial properties. In silico molecular docking experiments were performed against specific enzyme targets from the fatty acid and nucleic acid biosynthesis pathways to uncover their probable bactericidal mechanisms.
Fig. 1 (a) Synthesis of cellulose nanocrystals, (b) schematic diagram of GO/CNC–TiO2 synthesis and (c) chemical structure of synthesized GO/CNC–TiO2 QDs. |
Fig. 2 (a) XRD patterns and (b–e) SAED patterns of CNC, TiO2 CNC/TiO2 and GO/CNC-doped TiO2 QDs, respectively. |
Fig. 3 (a) Absorption spectra of undoped and GO/CNC-doped TiO2 QDs, (b) band gap plot and (c) PL spectra. |
The absorption spectra of the synthesized samples measured using a UV-Vis spectrophotometer are shown in Fig. 3a. The absorption peaks of CNC and TiO2 were found at around 370 and 380 nm, respectively.34,36 The peaks between 360–420 nm in the GO/CNC-doped TiO2 are attributed to the π → π* transition of the atomic C–C ring and C–O bond. Moreover, the lone pairs of electrons enabling n → π* transitions resulted in a further redshift in the peaks (360–460 nm) in CNC:TiO2.38 The absorption range increased in the visible range upon doping GO in CNC–TiO2, showing improved light-harvesting ability. This can be attributed to the relatively easy excitation of the lone electrons in contrast to the bonded electrons, resulting in more n → π* as compared to π → π* transitions.25 A decrease in bandgap energy (Eg) from 3.2 to 2.96 eV was observed for the doped samples,34,36,39 which can be attributed to the quantum confinement effect and increase in particle size upon GO/CNC doping in the control sample (Fig. 3b).40 Furthermore, efficiency of electron–hole pair recombination was characterized through photoluminescence spectrum, where a lower peak intensity designates a lower exciton recombination rate and effective dissociation of charge carriers, leading to an efficient photocatalytic performance. At the excitation wavelength of λmax = 300 nm, various emission peaks were observed, as shown in Fig. 3c. The extremely small size of the synthesized QDs compliment the quantum confinement effect, which is prominent in the PL emission spectra, given that energy level quantization and band gap reduction are major consequences of confinement in QDs.41 The PL emission spectrum of CNC with peaks positioned near 353, 410, and 465 nm and its contributions to the total spectrum are highly dependent on λex, which can be attributed to the carbonyl groups and various low-molecular derivatives of CNC.42 The PL spectra with peaks at 341, 400, 440, 467, and 488 nm for TiO2 and the doped samples are ascribed to oxygen vacancies and excitons (self-trapped) localized on TiO6 octahedra.43 The defect PL intensity was quenched when the Ti+ ions were irradiated with light due to the disorder and turbulence in the lattice, agreeing well with the Raman spectra of the GO/CNC:TiO2 QDs. The peak intensity of TiO2 was higher compared to that of CNC:TiO2, suggesting that exciton recombination was sharply reduced and electrons with a longer life were generated. The GO/CNC:TiO2 sample exhibited the lowest PL intensity, indicating the highest charge carrier separation efficiency and superior photocatalytic activity.44
Additionally, the structural and chemical properties were determined by analyzing the Raman spectra of all the prepared samples (Fig. 4a). A strong Raman band centered at ∼1005 cm−1 and numerous weak bands were observed at ∼200 to 670 cm−1, confirming the presence of CNC in the mapped area. The band observed at ∼1005 cm−1 is ascribed to the β-1,4 glycosidic linkage (C–O–C) stretching modes and C–O ring stretching modes of the glucose rings present in the cellulose chains.45 Furthermore, the bands detected at ∼200–670 cm−1 are ascribed to the skeletal bending ((CCC, COC, and OCC)) and stretching (CC and CO) modes, confirming the formation of CNC.46 Eg(1), B1g(1), A1(g) + B1g(2), and Eg(2) are the Raman vibrational mode matching symmetries, corresponding to the crystalline anatase TiO2 phase.47 Upon the doping of GO/CNC, a decrease in band intensity was also observed. The peaks detected at 1585 cm−1 (G band) and 1345 cm−1 (D band) also indicate the existence of the GO/CNC composites. The D band suggests the presence of sp3 defects in carbon atoms and the G peak gives information about the vibrations of the in-plane CC (sp2 hybridized) bonds of carbon-based materials.48 An enhancement in the G and D bands was observed for the doped samples. Moreover, the high ID/IG ratio was attributed to the increased number of sp2 domains.49
Fig. 4 (a) Raman spectra and (b) FTIR analysis of pristine CNC, TiO2, CNC@TiO2, and GO/CNC co-doped TiO2. |
The FTIR spectra exhibited the attached functional groups, adsorbed molecules and impurities on surface-activated bonding, consistent with the molecular vibration modes (Fig. 4b). The transmission bands of CNC were observed at 3400 and 1110 cm−1, representing the aromatic bands. The characteristic peak appearing at 3340 cm−1 is ascribed to the O–H (acid) stretching bonding due to the hydrogen bonding hydroxyl group vibrations. The transmission peak found at 1110 cm−1 was obtained from the stretching vibration of the C–O–C pyranose ring.50 The broad band of TiO2 observed at 3432 and 1629 cm−1 indicated O–H and N–H groups, respectively, adsorbed on the sample surface. The presence of a strong band in the range of 1000–450 cm−1 revealed that the Ti–O–Ti stretching modes shifted towards lower wavenumbers as a result of the combined effects of the Ti–O–Ti and Ti–O–C vibrations, indicating that GO/CNC was successfully doped. This band shift confirms the chemical reaction between TiO2 (surface hydroxyl groups) and GO/CNC (functional groups).36,51
The morphology of the prepared samples was revealed through HR-TEM, as depicted in Fig. 5(a and b). The obtained images of CNC and TiO2 display the structure of the particles with higher agglomerations (Fig. 5a), while the HRTEM image of TiO2 shows mostly the homogeneous size of QDs with a few chunks present, as shown in Fig. 5b. It was observed that the inclusion of CNC and GO increased the diameter of the spherical QDs, which were surrounded by CNC and GO sheets Fig. 5(c and d), respectively. The material may have an excessive number of active sites for reactants, which can considerably increase its catalytic potential.52 Further, the size of TiO2 and the CNC QDs was examined using imaging software, which computed the estimated values of 1.52 to 10.04 nm and 1.02 to 3.17 nm in length, respectively.
The interlayer d-spacing was calculated using the Gatan Digital-Micrograph software using the HR-TEM images, as shown in Fig. 6a–d. The d-spacing value for the pristine TiO2 was 0.295 nm, which agreed well with the XRD results (Fig. 6a). The d-values for CNC, CNC:TiO2, and GO/CNC:TiO2 were calculated to be 0.301, 0.363, and 0.442 nm, respectively. These values correspond to the (101) plane and increased slightly (0.295–0.442 nm), as seen in Fig. 6c and d.53 Furthermore, the change in d-spacing is ascribed to GO/CNC doping in the TiO2 lattice.
Fig. 6 Calculated d-spacings using HR-TEM images of (a) CNC, (b) TiO2, (c) CNC:TiO2 and (d) GO/CNC:TiO2. |
EDS analysis yielded information regarding the surface elemental composition of GO/CNC-doped TiO2, as shown in Fig. S2(a–d)†. According to the binding energies, the EDS spectrum contains peaks of carbon, titanium, oxygen, sulfur, and other elements. CNC contained 11.6 wt% elemental impurities of sulfur together with the main components of titanium (32.2%), carbon (30.1%), and oxygen (39.2% and 60.5%), as shown in Fig. S2(a and b)†. The oxygen peaks detected in the doped TiO2 confirm the incorporation of CNC and GO ions in the TiO2 lattice network. The elemental impurity can be ascribed to the dialysis of the CNC-containing sulfate groups, while the remainder resulted from the acid (H2SO4) hydrolysis of the cellulose nanocrystals.54 The tetragonal structure of TiO2 was revealed by XRD and its crystalline nature was established through SAED profiles. FTIR spectroscopy revealed the existence of functional groups and TiO2 (450 cm−1) in the fingerprint region. The presence of dopants (GO and C) and evaluation of the element constitution Ti and O were confirmed by EDS. The aforementioned results show the effective doping of GO and CNC in TiO2 with a QD morphology.
The light-induced activity of the pristine and GO/CNC-doped TiO2 QDs is illustrated in Fig. 7. The absorbance presented as a function of time in Fig. 7a shows the enhanced MB/MV/CF removal over GO/CNC–TiO2. It was noticed that the GO/CNC-doped TiO2 achieved the highest MB/MV/CF reduction, i.e., GO/CNC:TiO2, among the samples (Fig. 7c). The decrease in the recombination rate of excitons in GO/CNC:TiO2 is responsible for the improved photocatalytic activity of this system. The binary doping of GO and CNC may have induced defects in the lattice of TiO2 to act as trap sites for electrons, preventing them from reaching the holes. The PL spectra of the samples reflect this trend, with the pristine samples CNC and TiO2 having the maximum PL intensity, suggesting the highest recombination rate. PL peak intensity decreased for the binary-doped samples due to the slower exciton recombination in the lattice. The high photo-degradation efficiency may be due to the recombination of fewer excitons and increased visible light harvesting.
Fig. 7 Plot of ratio (Ct/C0) and −ln(Ct/Co) versus time for dye reduction (a) and (b), respectively. (c) Degradation% plot and (d) stability of co-doped TiO2 samples. |
The Langmuir–Hinshelwood model can help explain how organic dyes degrade. The adsorption of dye molecules on the catalyst surface is enhanced by an in increase in the surface area of the nanocomposites, which have a higher number of active sites. The irradiation of nanocatalysts produces es−–h+ pairs, which assist in redox reactions with the surrounding dye molecules. The photo-generated electrons reduce the dye molecules and the holes oxidize them, transforming them into less hazardous compounds. The lowest degradation activity was shown by the pristine sample (90%, 68.2% and 71.42%), while the highest degradation of 95.5%, 74.23% and 78.52% was exhibited by the binary-doped sample at pH = 7 (neutral), pH = 12 (basic) and pH = 7 (neutral), respectively, as shown in Fig. 7c and S3.† Furthermore, for comparison, dye degradation in the dark was investigated and the corresponding results are shown in Fig. S4.† The Langmuir–Hinshelwood model was used to evaluate the reaction rate constant.25 The equation ln(Ct/C0) = k was used to calculate the rate constants. The rate constants were attained from the slopes of the curves shown in Fig. 7b. For the undoped and doped samples, the calculated rate constants ranged from 0.1823 to 0.02346 min−1. Moreover, the dye concentration decreased continuously with an increase in the irradiation time.53 Experimental stability is a critical factor to be considered when evaluating a photocatalyst for wastewater treatment. The photocatalyst stability was examined by leaving the samples uninterrupted for three days and obtaining the absorption spectra from each sample every 24 h to record any variations in dye degradation. The degradation of the dye was monitored spectrophotometrically every 24 h and the corresponding results are depicted in Fig. 7d. The GO/CNC-doped TiO2 photocatalyst demonstrated outstanding stability and proved to be a promising photocatalyst.
The in vitro antimicrobial strength of the GO/CNC-doped TiO2 against E. coli and S. aureus retrieved from caprine mastitis fluid was evaluated. The findings show the superior additive antibacterial effect of GO/CNC-doped TiO2 against E. coli compared to S. aureus, as shown in Fig. S5.† The statistically important inhibitory areas (p < 0.05) were measured at a minimum and maximum dosage of (0.95 ± 0.05–1.03 ± 0.12 mm) and (1.67 ± 0.06–2.10 ± 0.05 mm) against S. aureus, while (3.36 ± 0.07–3.49 ± 0.05 mm) and (4.49 ± 0.05–5.21 ± 0.02 mm) against E. coli, respectively. TiO2 as a control specimen demonstrated a value of zero against E. coli at the minimum and maximum dosage. Ciprofloxacin decreased S. aureus and E. coli growth by (7.75 ± 0.00 mm) and (7.15 ± 0.00 mm), respectively, in contrast to DIW (0 ± 0.00 mm), as shown in Table S1.† The cumulative bactericidal potency of the GO/CNC-doped TiO2 material towards Gram-negative relative to Gram-positive was significant (p < 0.05). The oxidative damage generated by QDs depends on their form, concentration, and size, which are inversely proportional to the properties of the doped substances.55,56 The reactive oxygen species (ROS) released from QDs remain efficiently in the pathogen cell membrane, resulting in cytoplasmic extrusion and pathogen death.57 Secondly, the heavy cationic association of Ti4+ at higher concentrations with the negative pathogenic cell leads to cell deterioration and bacteria death.26
The use of computational techniques for mechanistic studies to rationalize the mystery behind biological activities and functions is well reported.26,34,58 Enzymes are considered to play the main role in bacterial infection, and thus inhibiting their activity serves to combat the caused infection.58,59 Here, the molecular docking predictions of TiO2–CNC and GO/CNC-doped TiO2 NPs against the FabI and DNA gyrase enzyme of E. coli and S. aureus revealed that they are the potent inhibitors of the given enzyme targets, as suggested by their binding tendency inside their binding pockets, respectively. The docked complex obtained for TiO2–CNC against FabI of E. coli revealed H-bonding with Ala21 (2.6 Å), Val14 (2.0 Å), and Ser19 (2.7 Å) having a binding score −9.117 kcal mol−1. The GO/CNC-doped TiO2 also showed a good binding score involving H-bond with Lys163 (2.4 Å and 2.5 Å) and Thr194 (2.5 Å) together with C–C interaction with Ser91 and Gly13, as depicted in Fig. S6.† The docked complex (−8.763 kcal mol−1) obtained for TiO2–CNC against FabI of S. aureus revealed the involvement of three amino acids, i.e., Ser44 (2.3 Å), Arg40 (2.4 Å and 2.8 Å) and Lys41 (2.4 Å), interacting through H-bonds, while GO/CNC-doped TiO2 revealed H-bonding with Ala95 (2.2 Å and 2.4 Å) and metal-contact with Ser197 (binding score of −5.974 kcal mol−1), as shown in Fig. S7.† Furthermore, the docking predictions for DNA gyrase from E. coli were also assessed to analyze the binding potential of TiO2–CNC (binding score: −6.849 kcal mol−1) and GO/CNC-doped TiO2 (binding score: −4.796 kcal mol−1) against active sites. The major interactions observed for TiO2–CNC were H-bonding with Asp73 (2.1 Å), Thr165 (1.8 Å), and Glu50 (2.5 Å), while GO/CNC-doped TiO2 interacted through H-bonding with Asp73 (2.0 Å) and Thr165 (1.7 Å), as depicted in Fig. 8.
Fig. 8 Binding interaction pattern of DNA gyrase from E. coli (a), TiO2–CNC (b), and GO/CNC-doped TiO2 (c) and superimposed docked complexes of TiO2–CNC and GO/CNC-doped TiO2 with DNA gyrase. |
Footnote |
† Electronic supplementary information (ESI) available. See https://doi.org/10.1039/d2na00383j |
This journal is © The Royal Society of Chemistry 2022 |