After the successful synthesis of nano photocatalysts has been placed in the sunlight, the photodegradation rate using methylene blue (MB) at starting dye concentrations of 10 mg per 500 ml is measured for 0.5 mg of photo-catalysts per 100 ml of dye solution. The samples' UV-vis wavelength spectrum was examined by subjecting them to varying durations of visible light exposure in order to determine their photocatalytic potential. The absorbance of the MB solution is measured at its highest absorption at a longer wavelength, of 465 nm for each distinct period of 15 min. The energy provided by sunlight as a level of intermediate excitation of electrons allowed the electrons in the Cr-doped TiO2 semiconductors to migrate from the valence band to the conduction band. When photogenerated holes and electrons move to the surface of nanocrystals (NCs), oxidative bases are formed. These NCs react by releasing adsorption-reacting agents which form hydroxyl (–OH) radicals, superoxide radicals, anions, and hydrogen peroxide, all of which contribute to the breakdown of dye. As the time frame of being subjected to direct sunlight increased to 120 minutes, a consistent rise in the degradation efficiency was seen for all fabricated samples, including pure, 0.3, and 0.5% Cr-doped TiO2 nanocrystals, as shown in Fig. 5 (a-c). Figures (5-a) illustrates the MB dye's gradual degradation caused by pure TiO2, which causes 21.4% of the dye to deteriorate in 120 minutes when exposed to sunshine. A substantial rise in MB degradation for 0.5% Cr-doped TiO2 nanocrystals is shown in Fig. 5 (c), with a degradation of 35.76% over the same 120-minute period. Figure 5 (d), which depicts the collective photodegradation efficiency of pure, 0.3, and 0.5% Cr-doped TiO2, shows how the MB dye degradation progressively increased over time. The degradation efficiency of all the fabricated samples was determined by using Eq. (2),
% Degradation Efficiency = \(\:\frac{{C}_{0}-\:{C}_{t}}{{C}_{0}}\:\times\:100\:\%\) ………………………… (2)
whereas C0 and Ct stand for the maximum absorbance at 465 nm for each generated sample, recorded under visible direct sunshine, at durations of 0 min and 15 min delay intervals up to 120 min (t). The Cr-doped TiO2 nanocrystals' exceptional photocatalytic performance is caused by their band gap shifting toward the visible spectrum. The TiO2 lattice's Cd doping could prolong the time that charge carriers stay preventing electron/hole recombination for a longer amount of time. Compared to pure TiO2, Cr-doped TiO2 produces new energy levels that increase photocatalytic activity and decrease the bandgap energy of the TiO2 nanocrystals. Cr doping produces oxygen vacancies, which operate as the most active locations for water splitting on the metal-doped TiO2 surfaces despite Cr2+ ions having a lower valency than Ti4+ ions. These reactive species play a major role in the decolorization of MB.
To understand how MB dye degrades photocatalytically, Fig. 6 (a,b) depicts the first-order model reaction kinetics of pure and Cr-doped TiO2. The kinetics of the first-order model is described by formula (3) below.
lnC0 / Ct = kt ……………………………………… (3)
Where C0 and Ct stand for the quantity of MB captured in direct sunlight for a total duration of 120 minutes at increments of 15 min. The symbols t and k stand for the reaction's time and rate constant, respectively. The linear fitting vs irradiation time of the photocatalytic degradation of MB was assessed using a tauc plot, as Fig. 6 (b) illustrates. The value of the predicted kinetic degradation rate constant (k) can be found by analyzing the gradient of the fitting curve. Under direct sunlight, it was observed that the computed values of (k) for pristine TiO2, and Cr-doped TiO2 are, respectively, (1.88, 1.98, and 2. 24) x 10− 3 min− 1 as illustrated in Table 2.
Photodegradation Mechanism
The Cr-doped TiO2 undergoes photoexcitation, which excites the electrons in the valence band (VB) to the conduction band (CB) and leaves the VB containing holes are shown in Fig. 7. Photons are absorbed and electron-hole pairs are generated; the electron-trapping effect of Cr ions prolongs the stability of the charge carriers by lowering the rate of recombination of these pairs. After migrating to the TiO2 particle's surface, the photogenerated electrons can convert molecular oxygen (O2) to produce superoxide radicals (O2•−). While the photogenerated holes move towards the surface, they can oxidize hydroxide ions (OH−) or water (H2O) and produce hydroxyl radicals (•OH). The methylene blue molecules are attacked by the hydroxyl radicals (•OH) and superoxide radicals (O2•−), which cause the complex organic structure of MB to break down into less destructive or environment-friendly molecules like CO2, H2O, and other least harmful inorganic ions. In the presence of Cr-doped TiO2, the entire photocatalytic degradation of methylene blue can be described by the following reaction:
MB + hν + O2 → CO2 + H2O + less destructive ions
The addition of Cr+ 3 ions to the TiO2 crystal lattice increases the pace of methylene blue breakdown overall because of enhanced charge carrier separation and extended light absorption towards the visible spectrum.
Table 3 presents a comparison of the current study to similar efforts in the literature already had been done by many researchers. The current study outperforms several earlier publications.