Basic magnesium sulfate@TiO2 composite for efficient adsorption and photocatalytic degradation of 4-dodecylmorpholine in brine

Basic magnesium sulfate@TiO2 composite for efficient adsorption and photocatalytic degradation of 4-dodecylmorpholine in brine | Research Square window.SnipcartSettings = { analytics: { enabled: false } }; (function() { var accessVector = localStorage.getItem('access_vector') || ''; window.dataLayer = window.dataLayer || []; if (accessVector) { window.dataLayer.push({ user: { profile: { profileInfo: { snid: accessVector } } } }); } })(); (function(w,d,s,l,i){w[l]=w[l]||[];w[l].push({'gtm.start':new Date().getTime(),event:'gtm.js'});var f=d.getElementsByTagName(s)[0],j=d.createElement(s),dl=l!='dataLayer'?'&l='+l:'';j.async=true;j.src='https://www.googletagmanager.com/gtm.js?id='+i+dl;f.parentNode.insertBefore(j,f);})(window,document,'script','dataLayer','GTM-K279D39R'); Browse Preprints In Review Journals COVID-19 Preprints AJE Video Bytes Research Tools Research Promotion AJE Professional Editing AJE Rubriq About Preprint Platform In Review Editorial Policies Our Team Advisory Board Help Center Sign In Submit a Preprint Cite Share Download PDF Article Basic magnesium sulfate@TiO 2 composite for efficient adsorption and photocatalytic degradation of 4-dodecylmorpholine in brine Zhongmei Song, Huifang Zhang, Liang Ma, Miao Lu, Chengyou Wu, and 6 more This is a preprint; it has not been peer reviewed by a journal. https://doi.org/ 10.21203/rs.3.rs-3892966/v1 This work is licensed under a CC BY 4.0 License Status: Published Journal Publication published 23 Apr, 2024 Read the published version in Scientific Reports → Version 1 posted 9 You are reading this latest preprint version Abstract More than 70% of the potash fertilizer globally is produced by the froth flotation process, in which 4-dodecylmorpholine (DMP) serves as a reverse flotation agent. As the potash fertilizer production rapidly rises, the increased DMP levels in discharged brine pose a threat to the production of high-value chemicals. In this paper, composite particles of basic magnesium sulfate@TiO2 (BMS@TiO2) were prepared using a simple and mild loading method. These particles were utilized for the adsorption and photocatalytic degradation of DMP in brine. Compared with normal powdered materials, the granular BMS@TiO2 in this study can be easily separated from liquid, and the degradation intermediates will not enter the brine without causing secondary pollution. BMS@TiO2 consists of 5·1·7 phase (5Mg(OH)2·MgSO4·7H2O) whisker clusters embedding 2.3% TiO2. The adsorption equilibrium of DMP on BMS@TiO2 particles was achieved through electrostatic attraction and pore interception with the adsorption capacity of approximately 5 mg·g-1 after 6 hours. The photodegradation efficiency of DMP adsorbed on BMS@TiO2 reached about 92% within 16 hours, which is compared with that of pure TiO2 nanoparticles. Additionally, excellent stability and recyclability of BMS@TiO2 were also observed in five cycle tests of adsorption and photocatalytic degradation of DMP, and the possible photocatalytic degradation pathways and mechanism of DMP are proposed following molecular electrostatic potential analysis. This work provides a sustainable and environmentally friendly approach for eliminating organic micropollutants from water environments. Earth and environmental sciences/Environmental sciences Physical sciences/Materials science Basic magnesium sulfate Adsorption Photocatalysis 4-dodecylmorpholine Degradation Figures Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7 Figure 8 Figure 9 Figure 10 Introduction Salt lakes contain large amounts of key minerals such as potassium and lithium, which are exploited for principally producing potash fertilizer, potassium nitrate for stored-heat molten salt, lithium carbonate in battery grade and so on. And these salt products are predominantly applied in agriculture and new energy, playing a vital role in promoting the economic and social development. Consequently, a series of steps are generally adopted to firstly extract potassium by flotation, and then lithium by membrane successively for sufficiently improving the comprehensive utilization efficiency of natural resources in salt lakes. Nevertheless, with the separation and enrich of potash resources forward, thousands of tons of flotation agents inevitably remain in potassium salt products, the effluent brine and the environment annually. In particular, the residues of flotation agent bring great challenges to the purification of products [1], and simultaneously increase the risk of membrane fouling in the subsequent procedures for extract lithium [2]. 4-dodecylmorpholine (DMP) is commonly used as a flotation collector in the reverse froth flotation procedure [3], and else assessed as secondary pollutant to ecological environment [4]. Therefore, the removal of DMP is necessary for further purification of related products and an important measure to protect the ecological environment. The primary techniques for eliminating organic matter in wastewater include natural sedimentation [5], coagulation [6], biological treatment [7], advanced oxidation [8], and adsorption [9]. The study about the photocatalytic oxidation performance of titanium dioxide for the degradation of DMP and octadecylamine (ODA), confirms the feasibility of photocatalytic oxidation for the removal of flotation agents [10]. However, the catalyst, usually in the form of a powder, results in unsatisfactory reuse performance, thus restricting its further application. Adsorption method can effectively separate organic micropollutant from brine, in most cases, also requires desorption and regeneration procedures, whereas photocatalytic oxidation can achieve degradation of the adsorbed organic micropollutants and regenerate the adsorption material without additional chemical regenerants [11, 12]. Therefore, the combination of the two methods is expected to enhance removal efficiency of organic micropollutants. Adsorbent materials, such as resin [13], metal-organic framework adsorbents [14], activated carbon [15], clay minerals [16-19] and molecular sieves [20] have been investigated extensively. Clay minerals, molecular sieves, and metal-organic frameworks are mostly in powder form, difficult to separate from liquids, while organic polymer resin may undergo aging by repeated illumination of ultraviolet light [21-24]. Activated carbon is often utilized as a carrier of photocatalysts for removing organic pollutants from wastewater. Liu et al. prepared an activated carbon photocatalyst supported by titanate nanotubes using the hydrothermal method to adsorb and photodegrade polycyclic aromatic hydrocarbons (PAHs). The maximum adsorption capacity was found to be 12.1 mg·g -1 , and PAHs could be photodegraded under ultraviolet light [25]. Zhu et al. developed an activated carbon composite supported by titanate nanotubes for removing perfluoro-2-propoxypropionic acid (GenX) with a photodegradation efficiency of 70% [26]. However, a long-term hydrothermal process [25-27] or calcination [28, 29] is typically required for the deposition of the photocatalyst onto the adsorbent materials, in which the loading efficiency of the photocatalyst is uncontrollable [30-32]. Cement-based materials are not only commonly used as building materials, but also can be doped with photocatalysts for photodegrading organic pollutants in water. Kumar et al. mixed BiVO 4 photocatalyst into Portland cement paste and coated it on the prepared concrete spheres for oxidative degradation of methylene blue with the degradation efficiency of 58% in 240 minutes under visible light [33]. He et al. introduced a self-made photocatalyst into Portland cement for photocatalytic oxidation of methyl orange, and the degradation efficiency of methyl orange was approximately 50 ~ 65% under ultraviolet irradiation [34]. Zhou et al. spread the photocatalyst K-g-C 3 N 4 powder onto the surface of uncured Portland cement and covered it with a glass slide for loading photocatalyst onto the cement surface [35]. The loading process of the photocatalyst on the above cement-based materials is mild and easy to operate. However, Portland cement is weakened and disintegrated by chemical reactions involving base exchange and the consequent leaching out of essential hydraulic components of the structure in salt solution [36]. Basic magnesium sulfate (BMS) possesses numerous distinct advantages, including high strength, light weight, good salt resistance, and hydrothermal resistance [37, 38]. However, there is little publication available regarding BMS doped with photocatalysts for photodegrading DMP flotation agents in brine. Herein, we have developed a facile approach to prepare BMS@TiO 2 composite with controllable TiO 2 loading and easy solid-liquid separation. In order to prevent possible degradation intermediates into brine, resulting in secondary pollution, BMS@TiO 2 particles after adsorbing DMP were separated from solution, and then were directly irradiated by ultraviolet light for photodegrading DMP. Combined with textural and electrochemical characterization, a series of experiments were performed to investigate and elucidate the adsorption and photodegradation performance of BMS@TiO 2 particles toward DMP in brine. Compared with commercial TiO 2 powder, BMS@TiO 2 particle only containing 2.3% TiO 2 presents similar adsorption and photocatalytic degradation efficiency, as well as more efficient reusability. This work will provide new fabrication strategies for developing composite photocatalysts convenient for large-scale application in the future. Materials And Methods Chemicals Basic magnesium carbonate (Mg(OH) 2 ·4MgCO 3 ·xH 2 O) was purchased from Beijing Mairuida Technology Co., Ltd (Beijing, China). Magnesium sulfate (MgSO 4 ·7H 2 O) was purchased from Tianjin Fengchuan Chemical Reagent Technology Co., Ltd (Tianjin, China). Citric acid monohydrate (C 6 H 8 O 7 ) was purchased from Tianjin Hengxing Chemical Reagent Manufacturing Co., Ltd (Tianjin, China). Manganese dioxide (MnO 2 ) was purchased from Tianjin Baishi Chemical Co., Ltd (Tianjin, China). Hydrogen peroxide (H 2 O 2 , 30%) was purchased from Tianjin Damao Chemical Reagent Factory (Tianjin, China). Methylorange (C 14 H 14 N 3 NaOS) was purchased from Beijing Reagent Factory (Beijing, China). Hydrochloric acid (HCl, 37%) was purchased from Sichuan Xi Long Chemical Co., Ltd (Sichuan, China). Sodium hydroxide (NaOH) was purchased from Xi’an Chemical Reagent Factory (Xi’an, China). 1,2-dichloroethane (1,2-ClCH 2 CH 2 Cl), glacial acetic acid (CH 3 COOH), anhydrous sodium acetate (CH 3 COONa), titanium dioxide (TiO 2 , anatase phase) and calcium stearate (C 36 H 70 CaO 4 ) were purchased from Shanghai Mclean Biochemical Technology Co., Ltd (Shanghai, China). All chemicals were of analytical grade or higher. Besides, 4-dodecylmorpholine (C 16 H 33 NO) was industrial grade and provided by the Qinghai Salt Lake Industry Co., Ltd (Qinghai, China). Table S1 of the supplementary information (SI) presents the physicochemical properties of 4-dodecylmorpholine. Synthesis of BMS@TiO 2 BMS@TiO 2 was synthesized using a facile method displayed in Fig.1. Firstly, 5 g of laboratory-prepared active magnesium oxide from basic magnesium carbonate, 0.5 g of TiO 2 , 0.015 g of calcium stearate, 0.025 g of citric acid, and 0.002 g of MnO 2 were mixed in a mold. Then, the mixture powder was combined with 16 g of a 25% magnesium sulfate solution and quickly whisked to form a uniform slurry. Finally, 1.5 g of a 30% H 2 O 2 solution was added into the mixture slurry to induce foaming until the mixture was solidified. The solid sample obtained after demoulding and constant solidifying for 7 days at room temperature condition, was labeled as BMS@TiO 2 and sieved to 20-60 mesh for adsorption and photocatalytic degradation experiments. Characterization The surface morphology and elemental mapping of the samples were examined by scanning electron microscopy (SEM, SU8010, Hitachi, Japan) equipped with energy-dispersive X-ray spectroscopy (EDS). The microstructure was observed via transmission electron microscopy (TEM, F200, Jeol Ltd.). The crystal phases of the samples were analyzed using X-ray diffraction (XRD-6000, Shimadzu) with Cu-Kα irradiation. The porous characteristics and the specific surface area (S BET ) were determined by the N 2 adsorption/desorption method at a NOVA2200e instrument (Quantachrome). The electronic properties were measured through the electron paramagnetic resonance spectrometer (EPR, A300, Bruker, Germany). The UV-vis diffuse reflectance spectrometry (UV-DRS) analysis was performed on a Lambda750UV/VIS spectrophotometer. The chemical functional groups of prepared samples were analyzed by a Fourier-transform infrared spectrophotometer (FTIR, Bruker TENSOR37, USA). Total organic carbon (TOC) was recorded with a TOC analyzer (Analytikyena, C/N3100, Germany). The electrochemical measurements were performed on a Wuhan Coster electrochemical workstation (CS310H) with a conventional three-electrode cell. Photometric determination of DMP Under a weak acidic environment, a 1:1 coordination reaction can occur between DMP and methyl orange. The product is bright yellow and soluble in 1,2-dichloroethane. When DMP remains in the lower organic phase and methyl orange enters the upper aqueous phase, the product will decompose under strong acidic conditions [39, 40]. In the wavelength range of 450~550 nm, the acid methyl orange produced by decomposition exhibits a unique absorption peak. Quantitative measurement of DMP concentration can be done using a linear relationship between absorbance and DMP concentration (Fig. S1(a)). A calibration based on the Beer-Lambert law was used to quantify the concentrations of DMP. A detailed description of the analysis is provided in the supplementary materials, and the standard curve is shown in Fig. S1(b). Adsorption experiment The adsorption capacities of BMS@TiO 2 for DMP were observed experimentally. Adsorption experiments were conducted by adding 0.1 g of BMS@TiO 2 particles in 50 mL of DMP solution in a dark environment with variations in adsorption time (0, 0.5, 1, 1.5, 2, 3, 4, 5, 6, 8, 12, 16, 20, 24, and 32 hours), operating temperature (25, 35, and 45℃), initial concentration (15, 20, 25, 30, and 35 mg·L -1 ), and co-existing salt (NaCl, KCl, and MgCl 2 ). Concentrations of DMP before and after adsorption were determined by the UV-vis spectrophotometer, and the absorption capacity ( q t , mg·g -1 ) of DMP on materials and removal efficiency ( R , %) were calculated via: where C t (mg·g -1 ) is the concentration of DMP at time t (h), C 0 and C e (mg·L -1 ) are the initial and equilibrium concentrations of DMP, respectively, V (L) is the total volume of the solution, and m (g) is the mass of adsorbent. Photocatalysis and Reuse of BMS@TiO 2 In order to prevent degradation intermediates into the solution, resulting in secondary pollution, BMS@TiO 2 particles after adsorbing DMP were separated from solution, and then directly irradiated for photodegrading DMP by ultraviolet light source of 280 ~ 380 nm (9 cm away from the light source) in a photocatalytic glass reactor with a quartz cover. After photocatalytic degradation, the particles were washed by water and dried at 30℃ for a duration of 12 hours for next adsorption experiment. The photocatalytic degradation rate ( η ) of DMP on BMS@TiO 2 was measured by dissolving the particles at a certain photodegradation time with 15 mL of a 1 mol·L -1 sulfuric acid solution, and calculated though the mathematical expression shown in formula (3). Pseudo-first-order and pseudo-second-order kinetic models were used to study the photocatalytic degradation behavior of DMP on BMS@TiO 2 , and the mathematical expressions are shown in formula (4) and (5) [41, 42]. Where m 0 and m t represent the mass of DMP on the BMS@TiO 2 at a certain photodegradation time (mg). k 1 (h -1 ), and k 2 (h·mg -1 ) are pseudo-first-order and pseudo-second-order kinetic model constants, respectively, and t is the photodegradation time (h). Results And Discussion Characterization of BMS@TiO 2 Surface morphology and chemical composition of BMS@TiO 2 The morphology of BMS and BMS@TiO 2 were characterized by SEM and TEM shown in Figs. 2(a) ~ 2(d). Both BMS and BMS@TiO 2 particles are mainly composed of irregular-crisscross whiskers, and their morphology is consistent with that of the 5·1·7 phase (5Mg(OH) 2 ·MgSO 4 ·7H 2 O) formed in the vent of the basic magnesium sulfate cement block [43]. Additionally, TiO 2 nanoparticle is combined with 5·1·7 phase, as evidenced by the lattice stripes of 5·1·7 phase and TiO 2 corresponding to the (222) and (101) planes respectively shown in Fig.2(d), which also demonstrates that TiO 2 can be firmly embedded in BMS substrate by the cement reactions between magnesium oxide and magnesium sulfate at room temperature. Figs. 2(e) ~ 2(h) display the element distribution of BMS and BMS@TiO 2 , and element composition is listed in Table S2. Obviously, TiO 2 is widely distributed in 5·1·7 phase matrix and enriched in some regions probably because of the inevitable agglomeration of TiO 2 nanoparticles during the synthesis process of BMS@TiO 2 . The content of titanium (Ti) in BMS@TiO 2 is 1.4% and the mass fraction of TiO 2 in BMS@TiO 2 is further calculated to be 2.3% approximately. Physical properties and structural characteristics of BMS@TiO 2 Figs. 3(a) and 3(b) show the FTIR spectra of BMS, TiO 2 , and BMS@TiO 2 . In the spectrum of TiO 2 , the vibration band at 3438 cm -1 indicates the presence of residual H 2 O molecules adsorbed on TiO 2 . Meanwhile, the stretching vibration peak at 1618 cm -1 corresponds to the bending vibration of O-H groups [44]. The strong band at 1012 cm -1 indicates the vibration of the Ti-O-Ti or Ti-O bond [45]. Furthermore, the vibration peak of Ti-O-Ti at 450 ~ 750 cm -1 is the anatase phase of TiO 2 [46, 47]. In BMS and BMS@TiO 2 , the peak at 3700 cm -1 occurs the stretching vibration of OH - , and the broad band peak at 3400 cm -1 is caused by the stretching vibration of crystal water (H-O), while the peak at 1636 cm -1 is due to the bending vibration of crystal water. The absorption band at 1450 cm -1 , which also appears in the infrared spectrum of magnesium hydroxide [48], probably corresponds to the asymmetric stretching vibration peak of Mg-OH. Likewise, the peak at 1103 cm -1 corresponds to the O 3 S-O stretching vibration peak of SO 4 2- . The peak at 617 cm -1 represents the stretching vibration peak of the S-O bond, while the subtle peak at 443 cm -1 corresponds to the stretching vibration peak of MgO-H [49-51], as well as the distinctive stretching vibration peak of Ti-O appears at 530 cm -1 in the BMS@TiO 2 spectrum. Furthermore, XRD patterns of BMS, TiO 2 , and BMS@TiO 2 in Fig. 3(c) also indicate that the predominant component both in BMS and BMS@TiO 2 is 5·1·7 phase, and the characteristic peaks at 9.44º, 17.80º, 30.83º, 36.15º and 37.34º belong to the distinctive features of 5·1·7 phase [52-54]. Besides, TiO 2 in BMS@TiO 2 exhibits distinct anatase features with characteristic peaks at 25.33º, 36.95º, 37.88º, 38.59º, 48.07º, 53.88º, 55.15º, 62.71º, as described in previous studies [45, 55]. The hysteresis characteristic and pore properties of BMS and BMS@TiO 2 were assessed using the N 2 adsorption-desorption method, and the results are depicted in Figs. 3(d) and 3(e). It can be proved that the hysteresis loops of BMS and BMS@TiO 2 exhibit typical IV isotherms with H3 hysteresis loops. This phenomenon possibly arises from the formation of slit-like pores among 5·1·7 phase whisker clusters [56]. The pore size distribution curves show that the major pore at 2.5 ~ 3.5 nm accompanied at approximately 20 nm appear in BMS and BMS@TiO 2 , and the specific surface area of BMS@TiO 2 is about 37 m 2 ·g -1 similar to that of BMS presented in Table S3. It is conceivable that the macroscopical gas hole formed during the foaming step by hydrogen peroxide and the microcosmic slit-like pores formed by 5·1·7 whisker clusters endow BMS@TiO 2 with a large specific surface area, which is beneficial to the adsorption and photocatalysis processes. The point of zero charges (PZC) of BMS, TiO 2 , and BMS@TiO 2 were measured by comparing the solution initial pH and final pH shown in Fig. 3(f), and the pH PZC values of BMS, TiO 2 , and BMS@TiO 2 are 11.54, 7.05, and 11.54, respectively. This is mainly because Mg-OH in basic magnesium sulfate is alkaline, making the interface negatively charged. Consequently, the physical properties and structural characteristics of basic magnesium sulfate material exhibited negligible alteration following the incorporation of TiO 2 . Optical properties of BMS@TiO 2 The optical properties of BMS, TiO 2 , and BMS@TiO 2 were evaluated using UV diffuse reflection spectroscopy (UV-DRS) and photoelectric signal detection, and the results are presented in Fig. 4. Compared with TiO 2 , BMS@TiO 2 also exhibits enhanced light absorption responses within 250 ~ 450 nm, and the absorbance exceeds 0.6, which is up to the half of pure TiO 2 . The band gap between the conduction and valence bands of the material is determined by the Tauc plots, as shown in formula (6) [57]. Where α is the absorbance value (a.u.), h is Planck's constant, v is the optical frequency, E g is the band gap energy (eV), and A is the constant. The value of n depends on the type of semiconductor material. TiO 2 (anatase) is an indirect transition semiconductor material, so the n value is 1/2. Fig. 4(b) illustrates that BMS@TiO 2 has a band gap energy at about 3.05 eV, similar to TiO 2 , and can be excited by ultraviolet light. Meanwhile, the steady-state surface photovoltage and transient photocurrent density are used to study the photoelectric conversion efficiency, that is, the separation and transfer efficiency of photogenerated charge and hole. In general, the higher the photovoltage and photocurrent, the stronger the photogenerated carrier transfer ability [58]. Fig. 4(c) and 4(d) show that all BMS, TiO 2 , and BMS@TiO 2 exhibits a certain photoelectric conversion ability, with the order of strength being TiO 2 ＞BMS@TiO 2 ＞BMS. As evidenced by Fig. 4, adding a small amount of TiO 2 (2.3%) significantly improved the photoelectric properties of basic magnesium sulfate, and thus BMS@TiO 2 has an appropriate photocatalytic ability. Adsorption study Fig. 5(a) shows the kinetics of DMP adsorption by BMS@TiO 2 . The adsorption equilibrium is reached after 6 hours, and the adsorption capacity is maintained at approximately 5.32 mg·g -1 in 1 mol·L -1 NaCl solution with an initial DMP concentration of 30 mg·L -1 . The model fitting parameters are shown in Table S4. The R 2 values for the pseudo-first-order and pseudo-second-order fitting were 0.9349 and 0.9907 with the theoretic maximum adsorption capacity to 5.51 and 5.49 mg·g -1 , respectively, suggesting the adsorption kinetics of BMS@TiO 2 for DMP can be accurately described by the pseudo-second-order model. Fig. 5(b) depicts the adsorption isotherm of DMP by BMS@TiO 2 , and the fitting parameters for Langmuir and Freundlich adsorption isotherm models are shown in Table S5. The results show that the adsorption data of BMS@TiO 2 are in good accord with the Langmuir isothermal model. Furthermore, the Langmuir equilibrium constants in milligrams are used in the Van't Hoff equation, and the values of Δ G , Δ H o , and Δ S o are obtained from Fig. 5(c) and summarized in Table S6. The negative Δ G values for different temperatures and the positive Δ H o value indicates that the adsorption process is endothermic and spontaneous. Furthermore, the influence of different co-existing salts and ionic strengths on the adsorption capacity are illustrated in Fig. 5(d). The general trend is that the adsorption capacity decreases with the increase of ionic strength. With the same ionic strength, the adsorption capacity of potassium chloride and sodium chloride changes to a similar extent. According to XRD patterns in Fig. S2, the phase composition of BMS@TiO 2 remains unchanged in both pure water and brine solution, exhibiting certain resistance to water and salt [59, 60]. There seems to because co-existing salts may affect the adsorption process, which in turn leads to a decrease in adsorption capacity. During the adsorption process, the adsorption solution pH value is approximately 6, so DMP is protonated in acidic condition shown as the chemical reaction (R1) [61] and becomes positively charged, while BMS@TiO 2 exhibits a negative surface charge known from the pH PZC value of 11.54. Further taking into account the structural characteristics of BMS@TiO 2 , the adsorption mechanism of DMP onto BMS@TiO 2 can be inferred as electrostatic interaction and pore interception. (R1) Consequently, the electrostatic interaction between DMP and BMS@TiO 2 is weakened due to the cationic shielding effect when the concentration of co-existing salts increase, resulting in the decrease of adsorption capacity [62]. Especially, the charge of Mg 2+ is higher than that of Na + and K + , resulting in a stronger charge shielding effect. On the other hand, cationic ions compete with DMP for water molecules, thereby reducing the affinity of DMP and water molecules, resulting in DMP easier to agglomerate and ultimately decreasing the critical micelle concentration (CMC) value of DMP. Therefore, the agglomerated DMP is not easily absorbed into BMS@TiO 2 by pore interception. Additionally, Mg 2+ has a stronger hydration capacity compare to Na + and K + , resulting in a more pronounced salting out effect, and the CMC value of DMP decreases more significantly when adding Mg 2+ [63, 64]. Fig. S3 shows SEM images, XRD patterns, FTIR spectra, and XPS full-scan spectra for BMS@TiO 2 before and after adsorption. The results indicate that in BMS@TiO 2 after adsorption, the 5·1·7 phase structure is still maintained, and regular whisker shape in SEM images are no longer present, which may be caused by the absorption of DMP onto 5·1·7 phase. Meanwhile, the corresponding FTIR spectra characteristic peaks of 5·1·7 phase do not significantly change before and after absorption, and the peaks at 2927 cm -1 and 2851 cm -1 appeared in the sample after adsorption are respectively assigned to the asymmetric ( ν a ) and symmetric ( ν s ) stretching modes of -CH 2 - groups in the organic adsorbate [65]. However, no new covalent bond signal is observed in FTIR spectra, indicating that the absorption of DMP by BMS@TiO 2 is a physical adsorption process. According to the XPS full-scan spectra of before and after absorption shown in Fig. 3S(d) and Table S7, it can be observed that the binding energy of Mg, O, Ti, and S on the surface of BMS@TiO 2 shift to varying degrees after adsorption, and especially the orbital binding energy offset of Mg, O, Ti, and S after adsorption is not enough to the extent of a chemical reaction, further indicating that the physical adsorption occurs on BMS@TiO 2 for DMP [66]. Additionally, the binding energy changes of Mg1s and O1s are 0.52 eV and 0.20 eV, respectively and comparatively significant, which indicate that DMP may interacts with MgO 6 octahedral skeleton of 5·1·7 phase in BMS@TiO 2 [67]. Photocatalytic degradation behavior and kinetic evaluation of DMP Fig. 6(a) demonstrates the adsorption capacity and photodegradation efficiency of DMP on BMS, TiO 2 , and BMS@TiO 2 . Compared with TiO 2 nanoparticles, 20-60 mesh BMS@TiO 2 particles with 2.3% TiO 2 exhibits an equally excellent adsorption and photocatalytic performance. Additionally, the photodegradation efficiency of DMP adsorbed on BMS particles reaches about 12%, which reveals that BMS also has weak photocatalytic activity, and this may be because BMS has weak light absorbance and some degree of photoelectric conversion efficiency shown in Fig. 4. Pseudo-first-order and pseudo-second-order kinetic models are employed to fit the photodegradation kinetics data of DMP on BMS@TiO 2 in Fig. 6(b), and the corresponding fitting parameters are listed in Table S8. The results indicate that the photodegradation equilibrium of DMP is reached after 16 hours and the photodegradation efficiency of DMP is approximately 92%. And photocatalytic kinetics of DMP on BMS@TiO 2 can be accurately represented by a pseudo-first-order kinetic model. In addition, as depicted in Fig. 6(c), FTIR spectra of BMS@TiO 2 before and after photodegradation at different time are obtained to verify the photodegradation kinetics behavior of DMP. The intensity of the peaks at 2927 cm -1 and 2851 cm -1 assigned to the asymmetric ( ν a ) and symmetric ( ν s ) stretching of -CH 2 - groups of the organic adsorbate gradually decreases with the extension of photodegradation time, adequately manifesting the photodegradation and removal of DMP adsorbed on BMS@TiO 2 . The total organic carbon (TOC) removal efficiency and GC-MS analysis of adsorbates on BMS@TiO 2 before and after photodegradation at different times shown in Fig. S4 are employed to further understand the photodegradation behavior of DMP. As the photodegradation time extends, TOC removal efficiency is up to 52% within 16 hours, distinctly lower than the photodegradation efficiency of DMP. According to the GC-MS analysis results of adsorbates on BMS@TiO 2 before and after photodegradation at 12 and 16 hours, there are at least three intermediates in industrial DMP, herein identified as I1, I2, and I3, respectively [68]. Moreover, DMP on BMS@TiO 2 thoroughly vanished by ultraviolet radiation at 16 hours, while the contents of these impurities slowly diminish. It is reasonable to conclude that DMP adsorbed on BMS@TiO 2 can be degraded and a small portion of impurities can also be adsorbed and photodegraded to varying degrees may because of their different degradability, limiting the apparent TOC removal efficiency. Stability and reusability of BMS@TiO 2 The consecutive adsorption and photodegradation tests for DMP on BMS@TiO 2 are conducted, and BMS@TiO 2 samples before and after cycle tests are analyzed by XRD, FTIR and N 2 adsorption/desorption method. The results obtained in Fig. 7 reveal that BMS@TiO 2 maintains a consistent adsorption performance with an average adsorption capacity of 5.33 mg·g -1 after five cycle tests, while the photocatalytic degradation efficiency gradually decreases from 92% at the first cycle to 81% at the fifth cycle. XRD patterns and pore characteristics of BMS@TiO 2 before and after cycle tests evidence that all of 5·1·7 phase, TiO 2 and the slit-pores at 2.5 ~ 3.5 nm accompanied at approximately 20 nm always exists, demonstrating that electrostatic interaction, pore interception and later photocatalysis of BMS@TiO 2 interacted with DMP steadily accomplished during cycle tests. Fig. 7(d) shows the FTIR spectra of BMS@TiO 2 before and after cycle tests. The corresponding characteristic peaks of BMS@TiO 2 remain unchanged, and peaks at 2927 cm -1 and 2851 cm -1 attributed to the asymmetric ( ν a ) and symmetric ( ν s ) stretching patterns of -CH 2 - groups appear after cycle tests. This is because, the residual impurities adsorbed on BMS@TiO 2 compete to consume active radicals in the next photodegradation, resulting in a decrease in the next apparent photocatalytic degradation efficiency. The degradation efficiency remained at approximately 81% in the third to fifth cycles shown in Fig. 7(a), which may be due to the residual quantity of impurities on BMS@TiO 2 reaching adsorption-degradation equilibrium at the cycle experimental conditions. Photodegradation mechanism of DMP by BMS@TiO 2 EPR spectra are conducted using 5,5-dimethyl-1-pyrroline N-oxide (DMPO) as the spin trapping agent in order to track the generation process of active species for degrading DMP adsorbed on BMS@TiO 2 . The remarkable characteristic peaks in Figs. 8(a) and 8(b) indicate respectively the formation of •OH and •O 2 - in BMS@TiO 2 photocatalytic system, which illustrates that the photodegradation removal of DMP adsorbed on BMS@TiO 2 is mainly accomplished by •OH and •O 2 - . And the signal intensity of all peaks gradually increases with the extension of exposure time, indicating the continuous generation of active species. The charge distribution and reactive sites of DMP are revealed by the electrostatic potential. This potential predicts the nucleophilic and electrophilic regions of the molecule, and negative and positive electrostatic potential regions favoring the occurrence of electrophilic attacks and nucleophilic attacks, respectively [69, 70]. As shown in Fig. 8(d), the electrostatic potential of DMP is visualized as red and blue surfaces surrounding the molecule. The blue color represents negative electrostatic potential values and the red color represents positive electrostatic potential values. The negative electrostatic potential region (blue colored) can be observed for the nitrogen and oxygen atoms located on the morpholine ring, and the positive electrostatic potential region (red colored) is located on the morpholine ring and the hydrogen atoms on C10 and C11 (Fig. 8(c)). Therefore, the nitrogen and oxygen atoms on the morpholine ring are susceptible to react with photogenerated holes and radicals, while the hydrogen atoms on the ring are susceptible to nucleophilic reaction. Based on the electrostatic potential of DMP and the intermediates, the possible reaction mechanism and degradation pathways of DMP by BMS@TiO 2 are proposed in Fig. 8(e). It is speculated that the hydrogen atoms on C17 of DMP are oxidized by the photogenerated radicals through nucleophilic reaction. As a result, the -CH 2 - group on the ring was oxidized and transformed into the C=O group [71]. Next, the generated P2 is oxidized by radicals h + , •OH, and •O 2 - to produce P3, which underwent rapid transformation to P4 through tautomerization. Groups -C 4 OH 7 in P4 are removed by radicals to form a long-chain alkane primary amine (P5) [72]. The primary amine (P5) is then progressively deaminated and demethylated to form P6 by radicals. Ultimately, these intermediate products may be broken down into small molecules and completely mineralize into CO 2 and H 2 O. The lack of inclusion of intermediates in the GC-MS at 12 and 16 hours is probably owing to their poor stability and susceptibility to degradation in the experimental conditions. As shown in Fig. 9, acute toxicity (as measured by the fathead minnow 50% lethal dose (LC 50 -96 h) and bioaccumulation factor are employed to evaluate the toxicities of DMP and the speculative photodegradation intermediates through the Toxicity Estimation Software Tool (T.E.S.T.) using the consensus method based on Quantitative Structure Activity Relationship (QSAR) prediction. Compared to DMP, the acute toxicities of intermediates tend to decrease when generating P1 and P2, then increase up until ensuing P3-P6, signifying that most intermediates are unfavored for reducing the toxicity and potential danger to the aqueous environment. The bioaccumulation factor exhibits similar pattern as acute toxicity, implying that only sufficient photocatalytic degradation and entire mineralization of DMP to CO 2 and H 2 O could alleviate the bioconcentration effect of DMP on the environment. Simultaneously, the impurities in industrial DMP, except I1, are more toxic and tendentious than DMP to bioconcentration effect. It is conceivable that the treatment procedures for adsorption of DMP and coexisting harmful impurities from brine and then photocatalytic degradation by BMS@TiO 2 in air could be an efficient and environmentally friendly approach to removing micropollutants, avoiding harmful intermediates enter the brine and cause secondary pollution. Fig. 10 summarizes the process of adsorption and photodegradation of DMP using BMS@TiO 2 . Conclusion In summary, the adsorption and photocatalytic degradation performances of BMS@TiO 2 composite for removing DMP from brine are explored thoroughly in this work. TiO 2 is firmly embedded in porous BMS substrate at room temperature with a loading content of 2.3%, as illustrated by the TEM images, the lattice stripe analysis, and the EDS results, respectively. In BMS@TiO 2 composite, the macroscopical gas hole formed during the foaming step by hydrogen peroxide and the microcosmic slit-like pores formed by 5·1·7 whisker clusters bring a specific surface area of about 37 m 2 ·g -1 , and it is advantageous to adsorption and photocatalysis. The adsorption of DMP on the surface of BMS@TiO 2 composite is realized through electrostatic attraction and pore interception, which can be revealed according to pH PZC , coexisting salt effect, and SEM images. The Langmuir isotherm and pseudo-second-order kinetics represent the most suitable isotherm and kinetic models for the adsorption process, which is essentially spontaneous and endothermic. Depending on the DRS, degradation efficiency, FTIR, and GC-MS analysis results, it is concluded that BMS@TiO 2 composite presents a similar photocatalytic degradation capability to pure TiO 2 powder with a band gap of 3.05 eV, and the degradation efficiency of DMP reaches 92% by direct UV irradiation for 16 h. Five consecutive cycles of adsorption and photocatalytic degradation experiments confirm that BMS@TiO 2 composite exhibits excellent absorption and photodegradation performance and reusability. EPR spectrua results verify the unremitting generation of radicals •OH and •O 2 - on BMS@TiO 2 interface by direct UV irradiation. Furthermore, the active reaction sites of DMP molecule are predicted by the electrostatic potential distribution calculation, and the photocatalytic degradation pathway is supposed to describe the photodegradation behavior of DMP. Therefore, our work proposes a facile approach for produce easy-recyclable and effective adsorbent and photocatalyst and safe removal treatment of DMP from brine. Declarations CRediT authorship contribution statement Z. S.: Data curation, Investigation, Writing-original draft. H. Z.: Formal analysis, Methodology, Writing-review & editing. L. M.: Methodology. M. L.: Formal analysis. C. W.: Conceptualization, Investigation, Methodology. Q. 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Ltd","correspondingAuthor":false,"prefix":"","firstName":"Xuefeng","middleName":"","lastName":"Yu","suffix":""},{"id":271549081,"identity":"1898727a-0a73-42c0-8205-c5f764c98c18","order_by":7,"name":"Haining Liu","email":"","orcid":"","institution":"                      , Qinghai Institute of Salt Lakes, Chinese Academy of Sciences","correspondingAuthor":false,"prefix":"","firstName":"Haining","middleName":"","lastName":"Liu","suffix":""},{"id":271549082,"identity":"a85bd54e-0846-4ff2-9182-01644ccf15b3","order_by":8,"name":"Xiushen Ye","email":"","orcid":"","institution":"                      , Qinghai Institute of Salt Lakes, Chinese Academy of Sciences","correspondingAuthor":false,"prefix":"","firstName":"Xiushen","middleName":"","lastName":"Ye","suffix":""},{"id":271549083,"identity":"fe412e9f-f531-4fe8-b8b9-f1a865481cf3","order_by":9,"name":"Zhen Ma","email":"","orcid":"","institution":"Qinghai Salt Lake Industry Co., Ltd","correspondingAuthor":false,"prefix":"","firstName":"Zhen","middleName":"","lastName":"Ma","suffix":""},{"id":271549084,"identity":"be7bca9a-d5d2-471d-bdcd-671699038dc8","order_by":10,"name":"Zhijian Wu","email":"","orcid":"","institution":"                      , Qinghai Institute of Salt Lakes, Chinese Academy of Sciences","correspondingAuthor":false,"prefix":"","firstName":"Zhijian","middleName":"","lastName":"Wu","suffix":""}],"badges":[],"createdAt":"2024-01-24 05:14:43","currentVersionCode":1,"declarations":"","doi":"10.21203/rs.3.rs-3892966/v1","doiUrl":"https://doi.org/10.21203/rs.3.rs-3892966/v1","draftVersion":[],"editorialEvents":[{"content":"https://doi.org/10.1038/s41598-024-59921-8","type":"published","date":"2024-04-23T22:49:51+00:00"}],"editorialNote":"","failedWorkflow":false,"files":[{"id":50854551,"identity":"4f39cf53-fe6d-49a9-a32f-50ef3b60400f","added_by":"auto","created_at":"2024-02-08 11:46:31","extension":"png","order_by":1,"title":"Figure 1","display":"","copyAsset":false,"role":"figure","size":306054,"visible":true,"origin":"","legend":"\u003cp\u003eSynthesis schematic diagram of BMS@TiO\u003csub\u003e2\u003c/sub\u003e\u003c/p\u003e","description":"","filename":"1.png","url":"https://assets-eu.researchsquare.com/files/rs-3892966/v1/c4d5036a70230a54399a3ea1.png"},{"id":50854552,"identity":"fde2d57c-20c7-4d5a-858f-c229b325855e","added_by":"auto","created_at":"2024-02-08 11:46:31","extension":"png","order_by":2,"title":"Figure 2","display":"","copyAsset":false,"role":"figure","size":871983,"visible":true,"origin":"","legend":"\u003cp\u003e(a, b) SEM images of BMS and BMS@TiO\u003csub\u003e2\u003c/sub\u003e, (c, d) TEM images of BMS@TiO\u003csub\u003e2\u003c/sub\u003e, (e, f) EDS spectra of BMS and BMS@TiO\u003csub\u003e2\u003c/sub\u003e, (g, h) EDS mapping images of BMS@TiO\u003csub\u003e2\u003c/sub\u003e.\u003c/p\u003e","description":"","filename":"2.png","url":"https://assets-eu.researchsquare.com/files/rs-3892966/v1/79c9f2379aaae3432ddb665b.png"},{"id":50854559,"identity":"548ffe69-6752-4577-8a74-162706c611f8","added_by":"auto","created_at":"2024-02-08 11:46:31","extension":"png","order_by":3,"title":"Figure 3","display":"","copyAsset":false,"role":"figure","size":265927,"visible":true,"origin":"","legend":"\u003cp\u003e(a) and (b) FTIR spectra of BMS, TiO\u003csub\u003e2\u003c/sub\u003e and BMS@TiO\u003csub\u003e2\u003c/sub\u003e, (c) XRD patterns of BMS, TiO\u003csub\u003e2\u003c/sub\u003e and BMS@TiO\u003csub\u003e2\u003c/sub\u003e, (d, e) N\u003csub\u003e2\u003c/sub\u003e adsorption-desorption isotherms and pore size distributions of BMS, and BMS@TiO\u003csub\u003e2\u003c/sub\u003e, (f) Point of zero charge (PZC) analysis of BMS, TiO\u003csub\u003e2\u003c/sub\u003e, and BMS@TiO\u003csub\u003e2\u003c/sub\u003e.\u003c/p\u003e","description":"","filename":"3.png","url":"https://assets-eu.researchsquare.com/files/rs-3892966/v1/93b95261be4a729b684d81f1.png"},{"id":50854555,"identity":"2634673a-94f8-47f9-9297-41dbcb098d4d","added_by":"auto","created_at":"2024-02-08 11:46:31","extension":"png","order_by":4,"title":"Figure 4","display":"","copyAsset":false,"role":"figure","size":212909,"visible":true,"origin":"","legend":"\u003cp\u003e(a) UV-DRS spectra, (b) Tauc plots analysis, (c) Surface photovoltage spectra, and (d) Transient photocurrent density spectra of BMS, TiO\u003csub\u003e2\u003c/sub\u003e, and BMS@TiO\u003csub\u003e2\u003c/sub\u003e.\u003c/p\u003e","description":"","filename":"4.png","url":"https://assets-eu.researchsquare.com/files/rs-3892966/v1/495119a058eadee0ed8cb2c5.png"},{"id":50855419,"identity":"e714f01e-dbaa-4cef-ba36-fa7cde37d812","added_by":"auto","created_at":"2024-02-08 11:54:31","extension":"png","order_by":5,"title":"Figure 5","display":"","copyAsset":false,"role":"figure","size":187283,"visible":true,"origin":"","legend":"\u003cp\u003e(a) Adsorption kinetics (\u003cem\u003eC\u003c/em\u003e\u003csub\u003e0\u003c/sub\u003e = 30 mg·L\u003csup\u003e-1\u003c/sup\u003e, \u003cem\u003eT\u003c/em\u003e = 25℃, \u003cem\u003eI\u003c/em\u003e\u003csub\u003eNaCl\u003c/sub\u003e = 1 mol·L\u003csup\u003e-1\u003c/sup\u003e, pH = 6.17), (b) Adsorption isotherms, (c) Van’t Hoff equation plot (ln \u003cem\u003eK\u003c/em\u003e\u003csub\u003e\u003cem\u003eeq\u003c/em\u003e\u003c/sub\u003e vs. 1/\u003cem\u003eT\u003c/em\u003e) to determine the thermodynamics parameter, (d) Effect of co-existing salts.\u003c/p\u003e","description":"","filename":"5.png","url":"https://assets-eu.researchsquare.com/files/rs-3892966/v1/dc956b468651928604d2ec78.png"},{"id":50854553,"identity":"b02aef74-65f1-4bf2-ae50-118fbf4e1b79","added_by":"auto","created_at":"2024-02-08 11:46:31","extension":"png","order_by":6,"title":"Figure 6","display":"","copyAsset":false,"role":"figure","size":298766,"visible":true,"origin":"","legend":"\u003cp\u003e(a) Adsorption capacity and photodegradation efficiency of DMP on BMS, TiO\u003csub\u003e2\u003c/sub\u003e, and BMS@TiO\u003csub\u003e2\u003c/sub\u003e, (b) Photodegradation kinetics, and (c) FTIR spectra of BMS@TiO\u003csub\u003e2\u003c/sub\u003e before and after photodegradation at different time.\u003c/p\u003e","description":"","filename":"6.png","url":"https://assets-eu.researchsquare.com/files/rs-3892966/v1/f80915965e9f148c510546f4.png"},{"id":50854561,"identity":"b076fe74-c6d5-435a-90be-910229ed6423","added_by":"auto","created_at":"2024-02-08 11:46:31","extension":"png","order_by":7,"title":"Figure 7","display":"","copyAsset":false,"role":"figure","size":385498,"visible":true,"origin":"","legend":"\u003cp\u003e(a) The cycle test of adsorption and photocatalytic performance of BMS@TiO\u003csub\u003e2\u003c/sub\u003e for removing DMP, (b) XRD patterns, (c) N\u003csub\u003e2\u003c/sub\u003e adsorption and desorption hysteresis loops, and (d) FTIR spectra of BMS@TiO\u003csub\u003e2\u003c/sub\u003e before and after cycle tests.\u003c/p\u003e","description":"","filename":"7.png","url":"https://assets-eu.researchsquare.com/files/rs-3892966/v1/127041bec56b4292ddbdd79b.png"},{"id":50854557,"identity":"5a12d12e-ebb8-4173-8d1e-3be25b4bbd88","added_by":"auto","created_at":"2024-02-08 11:46:31","extension":"png","order_by":8,"title":"Figure 8","display":"","copyAsset":false,"role":"figure","size":353806,"visible":true,"origin":"","legend":"\u003cp\u003e(a) EPR spectrum of DMPO-•OH, and (b) EPR spectrum of DMPO-•O\u003csub\u003e2\u003c/sub\u003e\u003csup\u003e-\u003c/sup\u003e in BMS@TiO\u003csub\u003e2\u003c/sub\u003e photocatalytic system, (c) Optimized structure of DMP at B3LYP-D3BJ/def2-SVPlevel, (d)Molecular electrostatic potential of DMP, (e) Proposed photodegradation pathways of DMP by BMS@TiO\u003csub\u003e2 \u003c/sub\u003eunder UV irradiation.\u003c/p\u003e","description":"","filename":"8.png","url":"https://assets-eu.researchsquare.com/files/rs-3892966/v1/c333611fa424b5e1879dd82e.png"},{"id":50854556,"identity":"0ddf6a2b-68de-4ac5-8c42-d7d7affa8a94","added_by":"auto","created_at":"2024-02-08 11:46:31","extension":"png","order_by":9,"title":"Figure 9","display":"","copyAsset":false,"role":"figure","size":88482,"visible":true,"origin":"","legend":"\u003cp\u003e(a) Acute toxicity of the fathead minnow LC\u003csub\u003e50\u003c/sub\u003e-96 h, and (b) Bioaccumulation factor of DMP and degradation intermediates predicted by T.E.S.T. based on the consensus method.\u003c/p\u003e","description":"","filename":"9.png","url":"https://assets-eu.researchsquare.com/files/rs-3892966/v1/7488a781a952da5a0ef50b30.png"},{"id":50854560,"identity":"39c61d55-834c-4b5b-b998-e8a75d116bf1","added_by":"auto","created_at":"2024-02-08 11:46:31","extension":"png","order_by":10,"title":"Figure 10","display":"","copyAsset":false,"role":"figure","size":496092,"visible":true,"origin":"","legend":"\u003cp\u003eAdsorption and photodegradation process of DMP by BMS@TiO\u003csub\u003e2\u003c/sub\u003e.\u003c/p\u003e","description":"","filename":"10.png","url":"https://assets-eu.researchsquare.com/files/rs-3892966/v1/fb6ee6d4f50739feb01d1bb5.png"},{"id":55691026,"identity":"63339687-f67d-4a45-bfb5-71b7d00a09f2","added_by":"auto","created_at":"2024-05-01 22:58:22","extension":"pdf","order_by":0,"title":"","display":"","copyAsset":false,"role":"manuscript-pdf","size":4143885,"visible":true,"origin":"","legend":"","description":"","filename":"manuscript.pdf","url":"https://assets-eu.researchsquare.com/files/rs-3892966/v1/9b172c91-984d-4b69-82d7-5771fb03e654.pdf"},{"id":50854554,"identity":"4161ec01-2378-43fe-9005-1bac99449c2e","added_by":"auto","created_at":"2024-02-08 11:46:31","extension":"docx","order_by":2,"title":"","display":"","copyAsset":false,"role":"supplement","size":1642060,"visible":true,"origin":"","legend":"","description":"","filename":"SupplementaryMaterial.docx","url":"https://assets-eu.researchsquare.com/files/rs-3892966/v1/44aa0806e491ea9e032a44f8.docx"}],"financialInterests":"No competing interests reported.","formattedTitle":"\u003cp\u003eBasic magnesium sulfate@TiO\u003csub\u003e2\u003c/sub\u003e composite for efficient adsorption and photocatalytic degradation of 4-dodecylmorpholine in brine\u003c/p\u003e","fulltext":[{"header":"Introduction","content":"\u003cp\u003eSalt lakes contain large amounts of key minerals such as potassium and lithium, which are exploited for principally producing potash fertilizer, potassium nitrate for stored-heat molten salt, lithium carbonate in battery grade and so on. And these salt products are predominantly applied in agriculture and new energy, playing a vital role in promoting the economic and social development. Consequently, a series of steps are generally adopted to firstly extract potassium by flotation, and then lithium by membrane successively for sufficiently improving the comprehensive utilization efficiency of natural resources in salt lakes.\u0026nbsp;Nevertheless, with the separation and enrich of potash resources forward, thousands of tons of flotation agents inevitably remain in potassium salt products, the effluent brine and the environment annually. In particular, the residues of flotation agent bring great challenges to the\u0026nbsp;purification\u0026nbsp;of\u0026nbsp;products [1], and simultaneously\u0026nbsp;increase the risk of membrane fouling in the subsequent procedures for extract lithium [2]. 4-dodecylmorpholine (DMP) is commonly used as a flotation collector in the reverse froth flotation procedure [3], and else assessed as secondary pollutant to ecological environment [4]. Therefore, the removal of DMP is necessary for further purification of related products and an important measure to protect the ecological environment.\u003c/p\u003e\n\u003cp\u003eThe primary techniques for eliminating organic matter in wastewater include natural sedimentation [5], coagulation [6], biological treatment [7], advanced oxidation [8], and adsorption [9]. The study about the photocatalytic oxidation performance of titanium dioxide for the degradation of DMP and octadecylamine (ODA), confirms the feasibility of photocatalytic oxidation for the removal of flotation agents [10]. However, the catalyst, usually in the form of a powder, results in unsatisfactory reuse performance, thus restricting its further application.\u0026nbsp;Adsorption method can effectively separate organic micropollutant from brine, in most cases, also requires desorption and regeneration procedures, whereas photocatalytic oxidation can achieve degradation of the adsorbed organic micropollutants and regenerate the adsorption material without additional chemical regenerants [11, 12]. Therefore, the combination of the two methods is expected to enhance removal efficiency of organic micropollutants.\u003c/p\u003e\n\u003cp\u003eAdsorbent materials, such as resin [13], metal-organic framework adsorbents [14], activated carbon [15], clay minerals [16-19] and molecular sieves [20] have been investigated extensively. Clay minerals, molecular sieves, and metal-organic frameworks are mostly in powder form, difficult to separate from liquids, while organic polymer resin may undergo aging by repeated illumination of ultraviolet light [21-24]. Activated carbon is often utilized as a carrier of photocatalysts for removing organic pollutants from wastewater. Liu et al. prepared an activated carbon photocatalyst supported by titanate nanotubes using the hydrothermal method to adsorb and photodegrade polycyclic aromatic hydrocarbons (PAHs). The maximum adsorption capacity was found to be 12.1 mg\u0026middot;g\u003csup\u003e-1\u003c/sup\u003e, and PAHs could be photodegraded under ultraviolet light [25]. Zhu et al. developed an activated carbon composite supported by titanate nanotubes for removing perfluoro-2-propoxypropionic acid (GenX) with a photodegradation efficiency of 70% [26]. However, a long-term hydrothermal process [25-27] or calcination [28, 29] is typically required for the deposition of the photocatalyst onto the adsorbent materials, in which the loading efficiency of the photocatalyst is uncontrollable [30-32].\u003c/p\u003e\n\u003cp\u003eCement-based materials are not only commonly used as building materials, but also can be doped with photocatalysts for photodegrading organic pollutants in water. Kumar et al. mixed BiVO\u003csub\u003e4\u003c/sub\u003e photocatalyst into Portland cement paste and coated it on the prepared concrete spheres for oxidative degradation of methylene blue with the degradation efficiency of 58% in 240 minutes under visible light [33]. He et al. introduced a self-made photocatalyst into Portland cement for photocatalytic\u0026nbsp;oxidation of methyl orange, and the degradation efficiency of methyl orange was approximately 50 ~ 65% under ultraviolet irradiation [34]. Zhou et al. spread the photocatalyst K-g-C\u003csub\u003e3\u003c/sub\u003eN\u003csub\u003e4\u003c/sub\u003e powder onto the surface of uncured Portland cement and covered it with a glass slide for loading photocatalyst onto the cement surface [35]. The loading process of the photocatalyst on the above cement-based materials is mild and easy to operate. However, Portland cement is weakened and disintegrated by chemical reactions involving base exchange and the consequent leaching out of essential hydraulic components of the structure in salt solution [36]. Basic magnesium sulfate (BMS) possesses numerous distinct advantages, including high strength, light weight, good salt resistance, and hydrothermal resistance [37, 38]. However, there is little publication available regarding BMS doped with photocatalysts for photodegrading DMP flotation agents in brine.\u003c/p\u003e\n\u003cp\u003eHerein, we have developed a facile approach to prepare BMS@TiO\u003csub\u003e2\u003c/sub\u003e composite with controllable TiO\u003csub\u003e2\u003c/sub\u003e loading and easy solid-liquid separation. In order to prevent possible degradation intermediates into brine, resulting in secondary pollution, BMS@TiO\u003csub\u003e2\u003c/sub\u003e particles after adsorbing DMP were separated from solution, and then were directly irradiated by ultraviolet light for photodegrading DMP. Combined with textural and electrochemical characterization, a series of experiments were performed to investigate and elucidate the adsorption and photodegradation performance of BMS@TiO\u003csub\u003e2\u003c/sub\u003e particles toward DMP in brine. Compared with commercial TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003epowder, BMS@TiO\u003csub\u003e2\u003c/sub\u003e particle only containing 2.3% TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003epresents similar adsorption and photocatalytic degradation efficiency, as well as more efficient reusability. This work will provide new fabrication strategies for developing composite photocatalysts convenient for large-scale application in the future.\u003c/p\u003e"},{"header":"Materials And Methods","content":"\u003cp\u003e\u003cstrong\u003eChemicals\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eBasic magnesium carbonate (Mg(OH)\u003csub\u003e2\u003c/sub\u003e\u0026middot;4MgCO\u003csub\u003e3\u003c/sub\u003e\u0026middot;xH\u003csub\u003e2\u003c/sub\u003eO) was purchased from Beijing Mairuida Technology Co., Ltd (Beijing, China). Magnesium sulfate (MgSO\u003csub\u003e4\u003c/sub\u003e\u0026middot;7H\u003csub\u003e2\u003c/sub\u003eO) was purchased from Tianjin Fengchuan Chemical Reagent Technology Co., Ltd (Tianjin, China). Citric acid monohydrate (C\u003csub\u003e6\u003c/sub\u003eH\u003csub\u003e8\u003c/sub\u003eO\u003csub\u003e7\u003c/sub\u003e) was purchased from Tianjin Hengxing Chemical Reagent Manufacturing Co., Ltd (Tianjin, China). Manganese dioxide (MnO\u003csub\u003e2\u003c/sub\u003e) was purchased from Tianjin Baishi Chemical Co., Ltd (Tianjin, China). Hydrogen peroxide (H\u003csub\u003e2\u003c/sub\u003eO\u003csub\u003e2\u003c/sub\u003e, 30%) was purchased from Tianjin Damao Chemical Reagent Factory (Tianjin, China). Methylorange (C\u003csub\u003e14\u003c/sub\u003eH\u003csub\u003e14\u003c/sub\u003eN\u003csub\u003e3\u003c/sub\u003eNaOS) was purchased from Beijing Reagent Factory (Beijing, China). Hydrochloric acid (HCl, 37%) was purchased from Sichuan Xi Long Chemical Co., Ltd (Sichuan, China). Sodium hydroxide (NaOH) was purchased from Xi\u0026rsquo;an Chemical Reagent Factory (Xi\u0026rsquo;an, China). 1,2-dichloroethane (1,2-ClCH\u003csub\u003e2\u003c/sub\u003eCH\u003csub\u003e2\u003c/sub\u003eCl), glacial acetic acid (CH\u003csub\u003e3\u003c/sub\u003eCOOH), anhydrous sodium acetate (CH\u003csub\u003e3\u003c/sub\u003eCOONa), titanium dioxide (TiO\u003csub\u003e2\u003c/sub\u003e, anatase phase) and calcium stearate (C\u003csub\u003e36\u003c/sub\u003eH\u003csub\u003e70\u003c/sub\u003eCaO\u003csub\u003e4\u003c/sub\u003e) were purchased from Shanghai Mclean Biochemical Technology Co., Ltd (Shanghai, China). All chemicals were of analytical grade or higher. Besides, 4-dodecylmorpholine (C\u003csub\u003e16\u003c/sub\u003eH\u003csub\u003e33\u003c/sub\u003eNO) was industrial grade and provided by the Qinghai Salt Lake Industry Co., Ltd (Qinghai, China). Table S1 of the supplementary information (SI) presents the physicochemical properties of 4-dodecylmorpholine.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eSynthesis of BMS@TiO\u003csub\u003e2\u003c/sub\u003e\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eBMS@TiO\u003csub\u003e2\u003c/sub\u003e\u003csub\u003e\u0026nbsp;\u003c/sub\u003ewas synthesized using a facile method displayed in Fig.1. Firstly, 5 g of laboratory-prepared active magnesium oxide from basic magnesium carbonate, 0.5 g of TiO\u003csub\u003e2\u003c/sub\u003e, 0.015 g of calcium stearate, 0.025 g of citric acid, and 0.002 g of MnO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003ewere mixed in a mold. Then, the mixture powder was combined with 16 g of a 25% magnesium sulfate solution and quickly whisked to form a uniform slurry. Finally, 1.5 g of a 30% H\u003csub\u003e2\u003c/sub\u003eO\u003csub\u003e2\u003c/sub\u003e solution was added into the mixture slurry to induce foaming until the mixture was solidified. The solid sample obtained after demoulding and constant solidifying for 7 days at room temperature condition, was labeled as BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003eand\u003csub\u003e\u0026nbsp;\u003c/sub\u003esieved to 20-60 mesh for adsorption and photocatalytic degradation experiments.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eCharacterization\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eThe surface morphology and elemental mapping of the samples were examined by scanning electron microscopy (SEM, SU8010, Hitachi, Japan) equipped with energy-dispersive X-ray spectroscopy (EDS). The microstructure was observed via transmission electron microscopy (TEM, F200, Jeol Ltd.). The crystal phases of the samples were analyzed using X-ray diffraction (XRD-6000, Shimadzu) with Cu-K\u0026alpha; irradiation. The porous characteristics and the specific surface area (S\u003csub\u003eBET\u003c/sub\u003e) were determined by the N\u003csub\u003e2\u003c/sub\u003e adsorption/desorption method at a NOVA2200e instrument (Quantachrome). The electronic properties were measured through the electron paramagnetic resonance spectrometer (EPR, A300, Bruker, Germany). The UV-vis diffuse reflectance spectrometry (UV-DRS) analysis was performed on a Lambda750UV/VIS spectrophotometer. The chemical functional groups of prepared samples were analyzed by a Fourier-transform infrared spectrophotometer (FTIR, Bruker TENSOR37, USA). Total organic carbon (TOC) was recorded with a TOC analyzer (Analytikyena, C/N3100, Germany). The electrochemical measurements were performed on a Wuhan Coster electrochemical workstation (CS310H) with a conventional three-electrode cell.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003ePhotometric determination of DMP\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eUnder a weak acidic environment, a 1:1 coordination reaction can occur between DMP and methyl orange. The product is bright yellow and soluble in 1,2-dichloroethane. When DMP remains in the lower organic phase and methyl orange enters the upper aqueous phase, the product will decompose under strong acidic conditions [39, 40]. In the wavelength range of 450~550 nm, the acid methyl orange produced by decomposition exhibits a unique absorption peak. Quantitative measurement of DMP concentration can be done using a linear relationship between absorbance and DMP concentration (Fig. S1(a)). A calibration based on the Beer-Lambert law was used to quantify the concentrations of DMP. A detailed description of the analysis is provided in the supplementary materials, and the standard curve is shown in Fig. S1(b).\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eAdsorption experiment\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eThe adsorption capacities of BMS@TiO\u003csub\u003e2\u003c/sub\u003e for DMP were observed experimentally. \u0026nbsp;Adsorption experiments were conducted by adding 0.1 g of BMS@TiO\u003csub\u003e2\u003c/sub\u003e particles in 50 mL of DMP solution in a dark environment with variations in adsorption time (0, 0.5, 1, 1.5, 2, 3, 4, 5, 6, 8, 12, 16, 20, 24, and 32 hours), operating temperature (25, 35, and 45℃), initial concentration (15, 20, 25, 30, and 35 mg\u0026middot;L\u003csup\u003e-1\u003c/sup\u003e), and co-existing salt (NaCl, KCl, and MgCl\u003csub\u003e2\u003c/sub\u003e). Concentrations of DMP before and after adsorption were determined by the UV-vis spectrophotometer, and the absorption capacity (\u003cem\u003eq\u003csub\u003et\u003c/sub\u003e\u003c/em\u003e, mg\u0026middot;g\u003csup\u003e-1\u003c/sup\u003e) of DMP on materials and removal efficiency (\u003cem\u003eR\u003c/em\u003e, %) were calculated via:\u003c/p\u003e\n\u003cp\u003e\u003cimg 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width=\"383\" height=\"93\"\u003e\u003c/p\u003e\n\u003cp\u003ewhere \u003cem\u003eC\u003csub\u003et\u003c/sub\u003e\u003c/em\u003e (mg\u0026middot;g\u003csup\u003e-1\u003c/sup\u003e) is the concentration of DMP at time t (h), \u003cem\u003eC\u003c/em\u003e\u003csub\u003e0\u003c/sub\u003e and\u003cem\u003e\u0026nbsp;C\u003csub\u003ee\u003c/sub\u003e\u003c/em\u003e (mg\u0026middot;L\u003csup\u003e-1\u003c/sup\u003e) are the initial and equilibrium concentrations of DMP, respectively, \u003cem\u003eV\u003c/em\u003e (L) is the total volume of the solution, and \u003cem\u003em\u003c/em\u003e (g) is the mass of adsorbent.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003ePhotocatalysis and Reuse of\u0026nbsp;\u003c/strong\u003e\u003cstrong\u003eBMS@TiO\u003csub\u003e2\u003c/sub\u003e\u003c/strong\u003e\u003cstrong\u003e\u0026nbsp;\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eIn order to prevent degradation intermediates into the solution, resulting in secondary pollution, BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003eparticles after adsorbing DMP were separated from solution, and then directly irradiated for photodegrading DMP by ultraviolet light source of 280 ~ 380 nm (9 cm away from the light source) in a photocatalytic glass reactor with a quartz cover. After photocatalytic degradation, the particles were washed by water and dried at 30℃ for a duration of 12 hours for next adsorption experiment. The photocatalytic degradation rate (\u003cem\u003e\u0026eta;\u003c/em\u003e) of DMP on BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003ewas measured by dissolving the particles at a certain photodegradation time with 15 mL of a 1 mol\u0026middot;L\u003csup\u003e-1\u003c/sup\u003e sulfuric acid solution, and calculated though the mathematical expression shown in formula (3). Pseudo-first-order and pseudo-second-order kinetic models were used to study the photocatalytic degradation behavior of DMP on BMS@TiO\u003csub\u003e2\u003c/sub\u003e, and the mathematical expressions are shown in formula (4) and (5) [41, 42].\u003c/p\u003e\n\u003cp\u003e\u003cimg src=\"data:image/png;base64,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\" width=\"401\" height=\"193\"\u003e\u003c/p\u003e\n\u003cp\u003eWhere \u003cem\u003em\u003c/em\u003e\u003csub\u003e0\u003c/sub\u003e and \u003cem\u003em\u003csub\u003et\u003c/sub\u003e\u003c/em\u003e represent the mass of DMP on the BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003eat a certain photodegradation time (mg).\u003cem\u003e\u0026nbsp;k\u003c/em\u003e\u003csub\u003e1\u003c/sub\u003e (h\u003csup\u003e-1\u003c/sup\u003e), and \u003cem\u003ek\u003c/em\u003e\u003csub\u003e2\u003c/sub\u003e (h\u0026middot;mg\u003csup\u003e-1\u003c/sup\u003e) are pseudo-first-order and pseudo-second-order kinetic model constants, respectively, and \u003cem\u003et\u003c/em\u003e is the photodegradation time (h).\u003c/p\u003e"},{"header":"Results And Discussion","content":"\u003cp\u003e\u003cstrong\u003eCharacterization of BMS@TiO\u003csub\u003e2\u003c/sub\u003e\u0026nbsp;\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003e\u003cem\u003eSurface morphology and chemical composition of BMS@TiO\u003csub\u003e2\u003c/sub\u003e\u003c/em\u003e\u003c/p\u003e\n\u003cp\u003eThe morphology of BMS and BMS@TiO\u003csub\u003e2\u003c/sub\u003e were characterized by SEM and TEM shown in Figs. 2(a) ~ 2(d). Both BMS and BMS@TiO\u003csub\u003e2\u003c/sub\u003e particles are mainly composed of irregular-crisscross whiskers, and their morphology is consistent with that of the 5\u0026middot;1\u0026middot;7 phase (5Mg(OH)\u003csub\u003e2\u003c/sub\u003e\u0026middot;MgSO\u003csub\u003e4\u003c/sub\u003e\u0026middot;7H\u003csub\u003e2\u003c/sub\u003eO) formed in the vent of the basic magnesium sulfate cement block [43]. Additionally, TiO\u003csub\u003e2\u003c/sub\u003e nanoparticle is combined with 5\u0026middot;1\u0026middot;7 phase, as evidenced by the lattice stripes of 5\u0026middot;1\u0026middot;7 phase and TiO\u003csub\u003e2\u003c/sub\u003e corresponding to the (222) and (101) planes respectively shown in Fig.2(d), which also demonstrates that TiO\u003csub\u003e2\u003c/sub\u003e can be firmly embedded in BMS substrate by the cement reactions between magnesium oxide and magnesium sulfate at room temperature. Figs. 2(e) ~ 2(h) display the element distribution of BMS and BMS@TiO\u003csub\u003e2\u003c/sub\u003e, and element composition is listed in Table S2. Obviously, TiO\u003csub\u003e2\u003c/sub\u003e is widely distributed in 5\u0026middot;1\u0026middot;7 phase matrix and enriched in some regions probably because of the inevitable agglomeration of TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003enanoparticles during the synthesis process of BMS@TiO\u003csub\u003e2\u003c/sub\u003e. The content of titanium (Ti) in BMS@TiO\u003csub\u003e2\u003c/sub\u003e is 1.4% and the mass fraction of TiO\u003csub\u003e2\u003c/sub\u003e in BMS@TiO\u003csub\u003e2\u003c/sub\u003e is further calculated to be 2.3% approximately.\u003c/p\u003e\n\u003cp\u003e\u003cem\u003ePhysical properties and structural characteristics of BMS@TiO\u003csub\u003e2\u003c/sub\u003e\u003c/em\u003e\u003c/p\u003e\n\u003cp\u003eFigs. 3(a) and 3(b) show the FTIR spectra of BMS, TiO\u003csub\u003e2\u003c/sub\u003e, and BMS@TiO\u003csub\u003e2\u003c/sub\u003e. In the spectrum of TiO\u003csub\u003e2\u003c/sub\u003e, the vibration band at 3438 cm\u003csup\u003e-1\u003c/sup\u003eindicates the presence of residual H\u003csub\u003e2\u003c/sub\u003eO molecules adsorbed on TiO\u003csub\u003e2\u003c/sub\u003e. Meanwhile, the stretching vibration peak at 1618 cm\u003csup\u003e-1\u0026nbsp;\u003c/sup\u003ecorresponds to the bending vibration of O-H groups [44]. The strong band at 1012 cm\u003csup\u003e-1\u003c/sup\u003e indicates the vibration of the Ti-O-Ti or Ti-O bond [45]. Furthermore, the vibration peak of Ti-O-Ti at 450 ~ 750 cm\u003csup\u003e-1\u003c/sup\u003e is the anatase phase of TiO\u003csub\u003e2\u003c/sub\u003e [46, 47]. In BMS and BMS@TiO\u003csub\u003e2\u003c/sub\u003e, the peak at 3700 cm\u003csup\u003e-1\u0026nbsp;\u003c/sup\u003eoccurs the stretching vibration of OH\u003csup\u003e-\u003c/sup\u003e, and the broad band peak at 3400 cm\u003csup\u003e-1\u003c/sup\u003e is caused by the stretching vibration of crystal water (H-O), while the peak at 1636 cm\u003csup\u003e-1\u003c/sup\u003e is due to the bending vibration of crystal water. The absorption band at 1450 cm\u003csup\u003e-1\u003c/sup\u003e, which also appears in the infrared spectrum of magnesium hydroxide [48], probably\u0026nbsp;corresponds to the asymmetric stretching vibration peak of Mg-OH. Likewise, the peak at 1103 cm\u003csup\u003e-1\u003c/sup\u003e corresponds to the O\u003csub\u003e3\u003c/sub\u003eS-O stretching vibration peak of SO\u003csub\u003e4\u003c/sub\u003e\u003csup\u003e2-\u003c/sup\u003e. The peak at 617 cm\u003csup\u003e-1\u0026nbsp;\u003c/sup\u003erepresents the stretching vibration peak of the S-O bond, while the subtle peak at 443 cm\u003csup\u003e-1\u003c/sup\u003e corresponds to the stretching vibration peak of MgO-H [49-51], as well as the distinctive stretching vibration peak of Ti-O appears at 530 cm\u003csup\u003e-1\u0026nbsp;\u003c/sup\u003ein the BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003espectrum. Furthermore, XRD patterns of BMS, TiO\u003csub\u003e2\u003c/sub\u003e, and BMS@TiO\u003csub\u003e2\u003c/sub\u003e in Fig. 3(c) also indicate that the predominant component both in BMS and BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003eis 5\u0026middot;1\u0026middot;7 phase, and the characteristic peaks at 9.44\u0026ordm;, 17.80\u0026ordm;, 30.83\u0026ordm;, 36.15\u0026ordm; and 37.34\u0026ordm; belong to the distinctive features of 5\u0026middot;1\u0026middot;7 phase [52-54]. Besides, TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003ein BMS@TiO\u003csub\u003e2\u003c/sub\u003e exhibits distinct anatase features with characteristic peaks at 25.33\u0026ordm;, 36.95\u0026ordm;, 37.88\u0026ordm;, 38.59\u0026ordm;, 48.07\u0026ordm;, 53.88\u0026ordm;, 55.15\u0026ordm;, 62.71\u0026ordm;, as described in previous studies [45, 55].\u003c/p\u003e\n\u003cp\u003eThe hysteresis characteristic and pore properties of BMS and BMS@TiO\u003csub\u003e2\u003c/sub\u003e were assessed using the N\u003csub\u003e2\u003c/sub\u003e adsorption-desorption method, and the results are depicted in Figs. 3(d) and 3(e). It can be proved that the hysteresis loops of BMS and BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003eexhibit typical IV isotherms with H3 hysteresis loops. This phenomenon possibly arises from the formation of slit-like pores among 5\u0026middot;1\u0026middot;7 phase whisker clusters [56]. The pore size distribution curves show that the major pore at 2.5 ~ 3.5 nm accompanied at approximately 20 nm appear in BMS and BMS@TiO\u003csub\u003e2\u003c/sub\u003e, and the specific surface area of BMS@TiO\u003csub\u003e2\u003c/sub\u003e is about 37 m\u003csup\u003e2\u003c/sup\u003e\u0026middot;g\u003csup\u003e-1\u003c/sup\u003e similar to that of BMS presented in Table S3. It is conceivable that the macroscopical gas hole formed during the foaming step by hydrogen peroxide and the microcosmic slit-like pores formed by 5\u0026middot;1\u0026middot;7 whisker clusters endow BMS@TiO\u003csub\u003e2\u003c/sub\u003e with a large specific surface area, which is beneficial to the adsorption and photocatalysis processes. The point of zero charges (PZC) of BMS, TiO\u003csub\u003e2\u003c/sub\u003e, and BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003ewere measured by comparing the solution initial pH and final pH shown in Fig. 3(f), and the pH\u003csub\u003ePZC\u003c/sub\u003e values of BMS, TiO\u003csub\u003e2\u003c/sub\u003e, and BMS@TiO\u003csub\u003e2\u003c/sub\u003e are 11.54, 7.05, and 11.54, respectively. This is mainly because Mg-OH in basic magnesium sulfate is alkaline, making the interface negatively charged. Consequently, the physical properties and structural characteristics of basic magnesium sulfate material exhibited negligible alteration following the incorporation of TiO\u003csub\u003e2\u003c/sub\u003e.\u003c/p\u003e\n\u003cp\u003e\u003cem\u003eOptical properties of BMS@TiO\u003csub\u003e2\u003c/sub\u003e\u003c/em\u003e\u003c/p\u003e\n\u003cp\u003eThe optical properties of BMS, TiO\u003csub\u003e2\u003c/sub\u003e, and BMS@TiO\u003csub\u003e2\u003c/sub\u003e were evaluated using UV diffuse reflection spectroscopy (UV-DRS) and photoelectric signal detection, and the results are presented in Fig. 4. Compared with TiO\u003csub\u003e2\u003c/sub\u003e, BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003ealso exhibits enhanced light absorption responses within 250 ~ 450 nm, and the absorbance exceeds 0.6, which is up to the half of pure TiO\u003csub\u003e2\u003c/sub\u003e. The band gap between the conduction and valence bands of the material is determined by the Tauc plots, as shown in formula (6) [57].\u003c/p\u003e\n\u003cp\u003e\u003cimg src=\"data:image/png;base64,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\" width=\"378\" height=\"38\"\u003e\u003c/p\u003e\n\u003cp\u003eWhere \u003cem\u003e\u0026alpha;\u003c/em\u003e is the absorbance value (a.u.), \u003cem\u003eh\u003c/em\u003e is Planck\u0026apos;s constant, \u003cem\u003ev\u003c/em\u003e is the optical frequency, \u003cem\u003eE\u003csub\u003eg\u003c/sub\u003e\u003c/em\u003e is the band gap energy (eV), and \u003cem\u003eA\u003c/em\u003e is the constant. The value of \u003cem\u003en\u003c/em\u003e depends on the type of semiconductor material. TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003e(anatase) is an indirect transition semiconductor material, so the \u003cem\u003en\u003c/em\u003e value is 1/2.\u003c/p\u003e\n\u003cp\u003eFig. 4(b) illustrates that BMS@TiO\u003csub\u003e2\u003c/sub\u003e has a band gap energy at about 3.05 eV, similar to TiO\u003csub\u003e2\u003c/sub\u003e, and can be excited by ultraviolet light. Meanwhile, the steady-state surface photovoltage and transient photocurrent density are used to study the photoelectric conversion efficiency, that is, the separation and transfer efficiency of photogenerated charge and hole. In general, the higher the photovoltage and photocurrent, the stronger the photogenerated carrier transfer ability\u0026nbsp;[58]. Fig. 4(c) and 4(d) show that all BMS, TiO\u003csub\u003e2\u003c/sub\u003e, and BMS@TiO\u003csub\u003e2\u003c/sub\u003e exhibits a certain photoelectric conversion ability, with the order of strength being TiO\u003csub\u003e2\u003c/sub\u003e＞BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003e＞BMS. As evidenced by Fig. 4, adding a small amount of TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003e(2.3%) significantly improved the photoelectric properties of basic magnesium sulfate, and thus BMS@TiO\u003csub\u003e2\u003c/sub\u003e has an appropriate photocatalytic ability.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eAdsorption study\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eFig. 5(a) shows the kinetics of DMP adsorption by BMS@TiO\u003csub\u003e2\u003c/sub\u003e. The adsorption equilibrium is reached after 6 hours, and the adsorption capacity is maintained at approximately 5.32 mg\u0026middot;g\u003csup\u003e-1\u003c/sup\u003e in 1 mol\u0026middot;L\u003csup\u003e-1\u003c/sup\u003e NaCl solution with an initial DMP concentration of 30 mg\u0026middot;L\u003csup\u003e-1\u003c/sup\u003e. The model fitting parameters are shown in Table S4. The \u003cem\u003eR\u003c/em\u003e\u003csup\u003e2\u003c/sup\u003e values for the pseudo-first-order and pseudo-second-order fitting were 0.9349 and 0.9907 with the theoretic maximum adsorption capacity to 5.51 and 5.49 mg\u0026middot;g\u003csup\u003e-1\u003c/sup\u003e, respectively, suggesting the adsorption kinetics of BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003efor DMP can be accurately described by the pseudo-second-order model. Fig. 5(b) depicts the adsorption isotherm of DMP by BMS@TiO\u003csub\u003e2\u003c/sub\u003e, and the fitting parameters for Langmuir and Freundlich adsorption isotherm models are shown in Table S5. The results show that the adsorption data of BMS@TiO\u003csub\u003e2\u003c/sub\u003e are in good accord with the Langmuir isothermal model. Furthermore, the Langmuir equilibrium constants in milligrams are used in the Van\u0026apos;t Hoff equation, and the values of \u0026Delta;\u003cem\u003eG\u003c/em\u003e, \u0026Delta;\u003cem\u003eH\u003c/em\u003e\u003csup\u003eo\u003c/sup\u003e, and \u0026Delta;\u003cem\u003eS\u003c/em\u003e\u003csup\u003eo\u003c/sup\u003e are obtained from Fig. 5(c) and summarized in Table S6. The negative \u0026Delta;\u003cem\u003eG\u003c/em\u003e values for different temperatures and the positive \u0026Delta;\u003cem\u003eH\u003c/em\u003e\u003csup\u003eo\u003c/sup\u003e value indicates that the adsorption process is endothermic and spontaneous.\u003c/p\u003e\n\u003cp\u003eFurthermore, the influence of different co-existing salts and ionic strengths on the adsorption capacity are illustrated in Fig. 5(d). The general trend is that the adsorption capacity decreases with the increase of ionic strength. With the same ionic strength, the adsorption capacity of potassium chloride and sodium chloride changes to a similar extent. According to XRD patterns in Fig. S2, the phase composition of BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003eremains unchanged in both pure water and brine solution, exhibiting certain resistance to water and salt [59, 60]. There seems to because co-existing salts may affect the adsorption process, which in turn leads to a decrease in adsorption capacity.\u003c/p\u003e\n\u003cp\u003eDuring the adsorption process, the adsorption solution pH value is approximately 6, so DMP is protonated in acidic condition shown as the chemical reaction (R1) [61] and becomes positively charged, while BMS@TiO\u003csub\u003e2\u003c/sub\u003e exhibits a negative surface charge known from the pH\u003csub\u003ePZC\u003c/sub\u003e value of 11.54. Further taking into account the structural characteristics of BMS@TiO\u003csub\u003e2\u003c/sub\u003e, the adsorption mechanism of DMP onto BMS@TiO\u003csub\u003e2\u003c/sub\u003e can be inferred as electrostatic interaction and pore interception.\u003c/p\u003e\n\u003cp\u003e\u003cimg 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\" alt=\"image\" width=\"654\" height=\"66\"\u003e\u0026nbsp; \u0026nbsp; \u0026nbsp; \u0026nbsp; \u0026nbsp;(R1)\u003c/p\u003e\n\u003cp\u003eConsequently, the electrostatic interaction between DMP and BMS@TiO\u003csub\u003e2\u003c/sub\u003e is weakened due to the cationic shielding effect when the concentration of co-existing salts increase, resulting in the decrease of adsorption capacity [62]. Especially, the charge of Mg\u003csup\u003e2+\u003c/sup\u003e is higher than that of Na\u003csup\u003e+\u003c/sup\u003e and K\u003csup\u003e+\u003c/sup\u003e, resulting in a stronger charge shielding effect. On the other hand, cationic ions compete with DMP for water molecules, thereby reducing the affinity of DMP and water molecules, resulting in DMP easier to agglomerate and ultimately decreasing the critical micelle concentration (CMC) value of DMP. Therefore, the agglomerated DMP is not easily absorbed into BMS@TiO\u003csub\u003e2\u003c/sub\u003e by pore interception. Additionally, Mg\u003csup\u003e2+\u003c/sup\u003e has a stronger hydration capacity compare to Na\u003csup\u003e+\u003c/sup\u003e and K\u003csup\u003e+\u003c/sup\u003e, resulting in a more pronounced salting out effect, and the CMC value of DMP decreases more significantly when adding Mg\u003csup\u003e2+\u0026nbsp;\u003c/sup\u003e[63, 64]. \u0026nbsp;\u003c/p\u003e\n\u003cp\u003eFig. S3 shows SEM images, XRD patterns, FTIR spectra, and XPS full-scan spectra for BMS@TiO\u003csub\u003e2\u003c/sub\u003e before and after adsorption. The results indicate that in BMS@TiO\u003csub\u003e2\u003c/sub\u003e after adsorption, the 5\u0026middot;1\u0026middot;7 phase structure is still maintained, and regular whisker shape in SEM images are no longer present, which may be caused by the absorption of DMP onto 5\u0026middot;1\u0026middot;7 phase. Meanwhile, the corresponding FTIR spectra characteristic peaks of 5\u0026middot;1\u0026middot;7 phase do not significantly change before and after absorption, and the peaks at 2927 cm\u003csup\u003e-1\u003c/sup\u003e and 2851 cm\u003csup\u003e-1\u003c/sup\u003e appeared in the sample after adsorption are respectively assigned to the asymmetric (\u003cem\u003e\u0026nu;\u003c/em\u003e\u003csub\u003ea\u003c/sub\u003e) and symmetric (\u003cem\u003e\u0026nu;\u003c/em\u003e\u003csub\u003es\u003c/sub\u003e) stretching modes of -CH\u003csub\u003e2\u003c/sub\u003e- groups in the organic adsorbate [65]. However, no new covalent bond signal is observed in FTIR spectra, indicating that the absorption of DMP by BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003eis a physical adsorption process. According to the XPS full-scan spectra of before and after absorption shown in Fig. 3S(d) and Table S7, it can be observed that the binding energy of Mg, O, Ti, and S on the surface of BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003eshift to varying degrees after adsorption, and especially the orbital binding energy offset of Mg, O, Ti, and S after adsorption is not enough to the extent of a chemical reaction, further indicating that the physical adsorption occurs on BMS@TiO\u003csub\u003e2\u003c/sub\u003e for DMP [66]. Additionally, the binding energy changes of Mg1s and O1s are 0.52 eV and 0.20 eV, respectively and comparatively significant, which indicate that DMP may interacts with MgO\u003csub\u003e6\u003c/sub\u003e octahedral skeleton of 5\u0026middot;1\u0026middot;7 phase in BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003e[67].\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003ePhotocatalytic degradation behavior and kinetic evaluation of DMP\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eFig. 6(a) demonstrates the adsorption capacity and photodegradation efficiency of DMP on BMS, TiO\u003csub\u003e2\u003c/sub\u003e, and BMS@TiO\u003csub\u003e2\u003c/sub\u003e. Compared with TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003enanoparticles, 20-60 mesh BMS@TiO\u003csub\u003e2\u003c/sub\u003e particles with 2.3% TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003eexhibits an equally excellent adsorption and photocatalytic performance. Additionally, the photodegradation efficiency of DMP adsorbed on BMS particles reaches about 12%, which reveals that BMS also has weak photocatalytic activity, and this may be because BMS has weak light absorbance and some degree of photoelectric conversion efficiency shown in Fig. 4. Pseudo-first-order and pseudo-second-order kinetic models are employed to fit the photodegradation kinetics data of DMP on BMS@TiO\u003csub\u003e2\u003c/sub\u003e in Fig. 6(b), and the corresponding fitting parameters are listed in Table S8. The results indicate that the photodegradation equilibrium of DMP is reached after 16 hours and the photodegradation efficiency of DMP is approximately 92%. And photocatalytic kinetics of DMP on BMS@TiO\u003csub\u003e2\u003c/sub\u003e can be accurately represented by a pseudo-first-order kinetic model. In addition, as depicted in Fig. 6(c), FTIR spectra of BMS@TiO\u003csub\u003e2\u003c/sub\u003e before and after photodegradation at different time are obtained to verify the photodegradation kinetics behavior of DMP. The intensity of the peaks at 2927 cm\u003csup\u003e-1\u003c/sup\u003e and 2851 cm\u003csup\u003e-1\u003c/sup\u003e assigned to the asymmetric (\u003cem\u003e\u0026nu;\u003c/em\u003e\u003csub\u003ea\u003c/sub\u003e) and symmetric (\u003cem\u003e\u0026nu;\u003c/em\u003e\u003csub\u003es\u003c/sub\u003e) stretching of -CH\u003csub\u003e2\u003c/sub\u003e- groups of the organic adsorbate gradually decreases with the extension of photodegradation time, adequately manifesting the photodegradation and removal of DMP adsorbed on BMS@TiO\u003csub\u003e2\u003c/sub\u003e. The total organic carbon (TOC) removal efficiency and GC-MS analysis of adsorbates on BMS@TiO\u003csub\u003e2\u003c/sub\u003e before and after photodegradation at different times shown in Fig. S4 are employed to further understand the photodegradation behavior of DMP. As the photodegradation time extends, TOC removal efficiency is up to 52% within 16 hours, distinctly lower than the photodegradation efficiency of DMP. According to the GC-MS analysis results of adsorbates on BMS@TiO\u003csub\u003e2\u003c/sub\u003e before and after photodegradation at 12 and 16 hours, there are at least three intermediates in industrial DMP, herein identified as I1, I2, and I3, respectively [68]. Moreover, DMP on BMS@TiO\u003csub\u003e2\u003c/sub\u003e thoroughly vanished by ultraviolet radiation at 16 hours, while the contents of these impurities slowly diminish. It is reasonable to conclude that DMP adsorbed on BMS@TiO\u003csub\u003e2\u003c/sub\u003e can be degraded and a small portion of impurities can also be adsorbed and photodegraded to varying degrees may because of their different degradability, limiting the apparent TOC removal efficiency.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eStability and reusability of BMS@TiO\u003csub\u003e2\u003c/sub\u003e\u0026nbsp;\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eThe consecutive adsorption and photodegradation tests for DMP on BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003eare conducted, and BMS@TiO\u003csub\u003e2\u003c/sub\u003e samples before and after cycle tests are analyzed by XRD, FTIR and N\u003csub\u003e2\u003c/sub\u003e adsorption/desorption method. The results obtained in Fig. 7 reveal that BMS@TiO\u003csub\u003e2\u003c/sub\u003e maintains a consistent adsorption performance with an average adsorption capacity of 5.33 mg\u0026middot;g\u003csup\u003e-1\u0026nbsp;\u003c/sup\u003eafter five cycle tests, while the photocatalytic degradation efficiency gradually decreases from 92% at the first cycle to 81% at the fifth cycle. XRD patterns and pore characteristics\u0026nbsp;of BMS@TiO\u003csub\u003e2\u003c/sub\u003e before and after cycle tests evidence that all of 5\u0026middot;1\u0026middot;7 phase, TiO\u003csub\u003e2\u003c/sub\u003e and the slit-pores at 2.5 ~ 3.5 nm accompanied at approximately 20 nm always exists, demonstrating that electrostatic interaction, pore interception and later photocatalysis of BMS@TiO\u003csub\u003e2\u003c/sub\u003e interacted with DMP steadily accomplished during cycle tests. Fig. 7(d) shows the FTIR spectra of BMS@TiO\u003csub\u003e2\u003c/sub\u003e before and after cycle tests. The corresponding characteristic peaks of BMS@TiO\u003csub\u003e2\u003c/sub\u003e remain unchanged, and peaks at 2927 cm\u003csup\u003e-1\u003c/sup\u003e and 2851 cm\u003csup\u003e-1\u003c/sup\u003e attributed to the asymmetric (\u003cem\u003e\u0026nu;\u003c/em\u003e\u003csub\u003ea\u003c/sub\u003e) and symmetric (\u003cem\u003e\u0026nu;\u003c/em\u003e\u003csub\u003es\u003c/sub\u003e) stretching patterns of -CH\u003csub\u003e2\u003c/sub\u003e- groups appear after cycle tests.\u0026nbsp;This is because, the residual impurities adsorbed on BMS@TiO\u003csub\u003e2\u003c/sub\u003e compete to consume active radicals in the next photodegradation, resulting in a decrease in the next apparent photocatalytic degradation efficiency. The degradation efficiency remained at approximately 81% in the third to fifth cycles shown in Fig. 7(a), which may be due to the residual quantity of impurities on BMS@TiO\u003csub\u003e2\u003c/sub\u003e reaching adsorption-degradation equilibrium at the cycle experimental conditions.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003ePhotodegradation mechanism of DMP by BMS@TiO\u003csub\u003e2\u003c/sub\u003e\u003c/strong\u003e\u0026nbsp;\u003c/p\u003e\n\u003cp\u003eEPR spectra are conducted using 5,5-dimethyl-1-pyrroline N-oxide (DMPO) as the spin trapping agent in order to track the generation process of active species for degrading DMP adsorbed on BMS@TiO\u003csub\u003e2\u003c/sub\u003e. The remarkable characteristic peaks in Figs. 8(a) and 8(b) indicate respectively the formation of \u0026bull;OH and \u0026bull;O\u003csub\u003e2\u003c/sub\u003e\u003csup\u003e-\u0026nbsp;\u003c/sup\u003ein BMS@TiO\u003csub\u003e2\u003c/sub\u003e photocatalytic system, which illustrates that the photodegradation removal of DMP adsorbed on BMS@TiO\u003csub\u003e2\u003c/sub\u003e is mainly accomplished by \u0026bull;OH and \u0026bull;O\u003csub\u003e2\u003c/sub\u003e\u003csup\u003e-\u003c/sup\u003e. And the signal intensity of all peaks gradually increases with the extension of exposure time, indicating the continuous generation of active species. The charge distribution and reactive sites of DMP are revealed by the electrostatic potential. This potential predicts the nucleophilic and electrophilic regions of the molecule, and negative and positive electrostatic potential regions favoring the occurrence of electrophilic attacks and nucleophilic attacks, respectively [69, 70]. As shown in Fig. 8(d), the electrostatic potential of DMP is visualized as red and blue surfaces surrounding the molecule. The blue color represents negative electrostatic potential values and the red color represents positive electrostatic potential values. The negative electrostatic potential region (blue colored) can be observed for the nitrogen and oxygen atoms located on the morpholine ring, and the positive electrostatic potential region (red colored) is located on the morpholine ring and the hydrogen atoms on C10 and C11 (Fig. 8(c)). Therefore, the nitrogen and oxygen atoms on the morpholine ring are susceptible to react with photogenerated holes and radicals, while the hydrogen atoms on the ring are susceptible to nucleophilic reaction.\u003c/p\u003e\n\u003cp\u003eBased on the electrostatic potential of DMP and the intermediates, the possible reaction mechanism and degradation pathways of DMP by BMS@TiO\u003csub\u003e2\u003c/sub\u003e are proposed in Fig. 8(e). It is speculated that the hydrogen atoms on C17 of DMP are oxidized by the photogenerated radicals through nucleophilic reaction. As a result, the -CH\u003csub\u003e2\u003c/sub\u003e- group on the ring was oxidized and transformed into the C=O group [71]. Next, the generated P2 is oxidized by radicals h\u003csup\u003e+\u003c/sup\u003e, \u0026bull;OH, and \u0026bull;O\u003csub\u003e2\u003c/sub\u003e\u003csup\u003e-\u003c/sup\u003e to produce P3, which underwent rapid transformation to P4 through tautomerization. Groups -C\u003csub\u003e4\u003c/sub\u003eOH\u003csub\u003e7\u003c/sub\u003e in P4 are removed by radicals to form a long-chain alkane primary amine (P5) [72]. The primary amine (P5) is then progressively deaminated and demethylated to form P6 by radicals. Ultimately, these intermediate products may be broken down into small molecules and completely mineralize into CO\u003csub\u003e2\u003c/sub\u003e and H\u003csub\u003e2\u003c/sub\u003eO. The lack of inclusion of intermediates in the GC-MS at 12 and 16 hours is probably owing to their poor stability and susceptibility to degradation in the experimental conditions.\u003c/p\u003e\n\u003cp\u003eAs shown in Fig. 9, acute toxicity (as measured by the fathead minnow 50% lethal dose (LC\u003csub\u003e50\u003c/sub\u003e-96 h) and bioaccumulation factor are employed to evaluate the toxicities of DMP and the speculative photodegradation intermediates\u003csub\u003e\u0026nbsp;\u003c/sub\u003ethrough the Toxicity Estimation Software Tool (T.E.S.T.) using the consensus method based on Quantitative Structure Activity Relationship (QSAR) prediction. Compared to DMP, the acute toxicities of intermediates tend to decrease when generating P1 and P2, then increase up until ensuing P3-P6, signifying that most intermediates are unfavored for reducing the toxicity and potential danger to the aqueous environment. The bioaccumulation factor exhibits similar pattern as acute toxicity, implying that only sufficient photocatalytic degradation and entire mineralization of DMP to CO\u003csub\u003e2\u003c/sub\u003e and H\u003csub\u003e2\u003c/sub\u003eO could alleviate the bioconcentration effect of DMP on the environment. Simultaneously, the impurities in industrial DMP, except I1, are more toxic and tendentious than DMP to bioconcentration effect. It is conceivable that the treatment procedures for adsorption of DMP and coexisting harmful impurities from brine and then photocatalytic degradation by BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003ein\u003csub\u003e\u0026nbsp;\u003c/sub\u003eair\u003csub\u003e\u0026nbsp;\u003c/sub\u003ecould be an efficient and environmentally friendly approach to removing micropollutants, avoiding harmful intermediates enter the brine and cause secondary pollution. Fig. 10 summarizes the process of adsorption and photodegradation of DMP using BMS@TiO\u003csub\u003e2\u003c/sub\u003e.\u003c/p\u003e"},{"header":"Conclusion","content":"\u003cp\u003eIn summary, the adsorption and photocatalytic degradation performances of BMS@TiO\u003csub\u003e2\u003c/sub\u003e composite for removing DMP from brine are explored thoroughly in this work. TiO\u003csub\u003e2\u003c/sub\u003e is firmly embedded in porous BMS substrate at room temperature with a loading content of 2.3%, as illustrated by the TEM images, the lattice stripe analysis, and the EDS results, respectively. In BMS@TiO\u003csub\u003e2\u003c/sub\u003e composite, the macroscopical gas hole formed during the foaming step by hydrogen peroxide and the microcosmic slit-like pores formed by 5\u0026middot;1\u0026middot;7 whisker clusters bring a specific surface area of about 37 m\u003csup\u003e2\u003c/sup\u003e\u0026middot;g\u003csup\u003e-1\u003c/sup\u003e, and it is advantageous to adsorption and photocatalysis. The adsorption of DMP on the surface of BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003ecomposite is realized through electrostatic attraction and pore interception, which can be revealed according to pH\u003csub\u003ePZC\u003c/sub\u003e, coexisting salt effect, and SEM images. The Langmuir isotherm and pseudo-second-order kinetics represent the most suitable isotherm and kinetic models for the adsorption process, which is essentially spontaneous and endothermic. Depending on the DRS, degradation efficiency, FTIR, and GC-MS analysis results, it is concluded that BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003ecomposite presents a similar photocatalytic degradation capability to pure TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003epowder\u003csub\u003e\u0026nbsp;\u003c/sub\u003ewith a band gap of 3.05 eV, and the degradation efficiency of DMP reaches 92% by direct UV irradiation for 16 h. Five consecutive cycles of adsorption and photocatalytic degradation experiments confirm that BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003ecomposite\u003csub\u003e\u0026nbsp;\u003c/sub\u003eexhibits excellent absorption and photodegradation performance and reusability. EPR spectrua results verify the unremitting generation of radicals \u0026bull;OH and \u0026bull;O\u003csub\u003e2\u003c/sub\u003e\u003csup\u003e-\u0026nbsp;\u003c/sup\u003eon BMS@TiO\u003csub\u003e2\u0026nbsp;\u003c/sub\u003einterface\u003csub\u003e\u0026nbsp;\u003c/sub\u003eby direct UV irradiation. Furthermore, the active reaction sites of DMP molecule are predicted by the electrostatic potential distribution calculation, and the photocatalytic degradation pathway is supposed to describe the photodegradation behavior of DMP. Therefore, our work proposes a facile approach for produce easy-recyclable and effective adsorbent and photocatalyst and safe removal treatment of DMP from brine.\u003c/p\u003e"},{"header":"Declarations","content":"\u003cp\u003e\u003cstrong\u003eCRediT authorship contribution statement\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eZ. S.: Data curation, Investigation, Writing-original draft. H. Z.: Formal analysis, Methodology, Writing-review \u0026amp; editing. L. M.: Methodology. M. L.: Formal analysis. C. W.: Conceptualization, Investigation, Methodology. Q. L.: Resources. X. Y.: Validation. H. L.: Resources, Supervision. X. Y.: Project administration. Z. M.: Resources. Z. W.: Conceptualization.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eDeclaration of Competing Interest\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eThe authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eAcknowledgment\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eThis work was financially supported by the financial support from the National Natural Science Foundation of China (U20A20150), Key Research \u0026amp; Development Plan of Qinghai Province (2023-GX-103), and Youth Science and Technology Talent Promotion of Qinghai Province (2021QHSKERCTJ11).\u003c/p\u003e"},{"header":"References","content":"\u003col\u003e\n\u003cli\u003eZhang, G., Dong, C.L., Feng, X.L. Effect of flotation agent in potassium chloride on potassium nitrate production process. \u003cem\u003eJ. Salt Sci. Chem. 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Technol.\u003c/em\u003e \u003cstrong\u003e53,\u003c/strong\u003e 1564-1575 (2019).\u003c/li\u003e\n\u003c/ol\u003e"}],"fulltextSource":"","fullText":"","funders":[],"hasAdminPriorityOnWorkflow":false,"hasManuscriptDocX":true,"hasOptedInToPreprint":true,"hasPassedJournalQc":"","hasAnyPriority":false,"hideJournal":false,"highlight":"","institution":"","isAcceptedByJournal":true,"isAuthorSuppliedPdf":false,"isDeskRejected":"","isHiddenFromSearch":false,"isInQc":false,"isInWorkflow":false,"isPdf":false,"isPdfUpToDate":true,"isWithdrawnOrRetracted":false,"journal":{"display":true,"email":"[email protected]","identity":"scientific-reports","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":false,"externalIdentity":"scirep","sideBox":"Learn more about [Scientific Reports](http://www.nature.com/srep/)","snPcode":"","submissionUrl":"","title":"Scientific Reports","twitterHandle":"","acdcEnabled":true,"dfaEnabled":true,"editorialSystem":"stoa","reportingPortfolio":"Scientific Reports","inReviewEnabled":true,"inReviewRevisionsEnabled":true},"keywords":"Basic magnesium sulfate, Adsorption, Photocatalysis, 4-dodecylmorpholine, Degradation","lastPublishedDoi":"10.21203/rs.3.rs-3892966/v1","lastPublishedDoiUrl":"https://doi.org/10.21203/rs.3.rs-3892966/v1","license":{"name":"CC BY 4.0","url":"https://creativecommons.org/licenses/by/4.0/"},"manuscriptAbstract":"More than 70% of the potash fertilizer globally is produced by the froth flotation process, in which 4-dodecylmorpholine (DMP) serves as a reverse flotation agent. As the potash fertilizer production rapidly rises, the increased DMP levels in discharged brine pose a threat to the production of high-value chemicals. In this paper, composite particles of basic magnesium sulfate@TiO2 (BMS@TiO2) were prepared using a simple and mild loading method. These particles were utilized for the adsorption and photocatalytic degradation of DMP in brine. Compared with normal powdered materials, the granular BMS@TiO2 in this study can be easily separated from liquid, and the degradation intermediates will not enter the brine without causing secondary pollution. BMS@TiO2 consists of 5·1·7 phase (5Mg(OH)2·MgSO4·7H2O) whisker clusters embedding 2.3% TiO2. The adsorption equilibrium of DMP on BMS@TiO2 particles was achieved through electrostatic attraction and pore interception with the adsorption capacity of approximately 5 mg·g-1 after 6 hours. The photodegradation efficiency of DMP adsorbed on BMS@TiO2 reached about 92% within 16 hours, which is compared with that of pure TiO2 nanoparticles. Additionally, excellent stability and recyclability of BMS@TiO2 were also observed in five cycle tests of adsorption and photocatalytic degradation of DMP, and the possible photocatalytic degradation pathways and mechanism of DMP are proposed following molecular electrostatic potential analysis. This work provides a sustainable and environmentally friendly approach for eliminating organic micropollutants from water environments.","manuscriptTitle":"Basic magnesium sulfate@TiO2 composite for efficient adsorption and photocatalytic degradation of 4-dodecylmorpholine in brine","msid":"","msnumber":"","nonDraftVersions":[{"code":1,"date":"2024-02-08 11:46:26","doi":"10.21203/rs.3.rs-3892966/v1","editorialEvents":[{"type":"communityComments","content":0},{"type":"decision","content":"Revision requested","date":"2024-03-01T05:23:45+00:00","index":"","fulltext":""},{"type":"editorInvitedReview","content":"","date":"2024-02-29T16:29:07+00:00","index":"hide","fulltext":""},{"type":"editorInvitedReview","content":"","date":"2024-02-21T12:23:59+00:00","index":"hide","fulltext":""},{"type":"reviewerAgreed","content":"931d62a5-475b-4172-8fb2-04d20a0d9ff8","date":"2024-02-08T08:06:43+00:00","index":"hide","fulltext":""},{"type":"reviewersInvited","content":"","date":"2024-02-08T04:33:13+00:00","index":"","fulltext":""},{"type":"editorAssigned","content":"","date":"2024-02-07T11:49:22+00:00","index":"","fulltext":""},{"type":"editorInvited","content":"","date":"2024-02-07T10:05:50+00:00","index":"","fulltext":""},{"type":"checksComplete","content":"","date":"2024-02-07T02:07:38+00:00","index":"","fulltext":""},{"type":"submitted","content":"Scientific Reports","date":"2024-01-24T05:01:37+00:00","index":"","fulltext":""}],"status":"published","journal":{"display":true,"email":"[email protected]","identity":"scientific-reports","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":false,"externalIdentity":"scirep","sideBox":"Learn more about [Scientific Reports](http://www.nature.com/srep/)","snPcode":"","submissionUrl":"","title":"Scientific Reports","twitterHandle":"","acdcEnabled":true,"dfaEnabled":true,"editorialSystem":"stoa","reportingPortfolio":"Scientific Reports","inReviewEnabled":true,"inReviewRevisionsEnabled":true}}],"origin":"","ownerIdentity":"b592881c-836d-48b7-96c4-c09696d0c120","owner":[],"postedDate":"February 8th, 2024","published":true,"recentEditorialEvents":[],"rejectedJournal":[],"revision":"","amendment":"","status":"published-in-journal","subjectAreas":[{"id":28653181,"name":"Earth and environmental sciences/Environmental sciences"},{"id":28653182,"name":"Physical sciences/Materials science"}],"tags":[],"updatedAt":"2024-05-01T22:49:51+00:00","versionOfRecord":{"articleIdentity":"rs-3892966","link":"https://doi.org/10.1038/s41598-024-59921-8","journal":{"identity":"scientific-reports","isVorOnly":false,"title":"Scientific Reports"},"publishedOn":"2024-04-23 22:49:51","publishedOnDateReadable":"April 23rd, 2024"},"versionCreatedAt":"2024-02-08 11:46:26","video":"","vorDoi":"10.1038/s41598-024-59921-8","vorDoiUrl":"https://doi.org/10.1038/s41598-024-59921-8","workflowStages":[]},"version":"v1","identity":"rs-3892966","journalConfig":"researchsquare"},"__N_SSP":true},"page":"/article/[identity]/[[...version]]","query":{"redirect":"/article/rs-3892966","identity":"rs-3892966","version":["v1"]},"buildId":"qtupq5eGEP_6zYnWcrvyt","isFallback":false,"isExperimentalCompile":false,"dynamicIds":[84888],"gssp":true,"scriptLoader":[]}