• <tr id="yyy80"></tr>
  • <sup id="yyy80"></sup>
  • <tfoot id="yyy80"><noscript id="yyy80"></noscript></tfoot>
  • 99热精品在线国产_美女午夜性视频免费_国产精品国产高清国产av_av欧美777_自拍偷自拍亚洲精品老妇_亚洲熟女精品中文字幕_www日本黄色视频网_国产精品野战在线观看 ?

    Pulsed gas-liquid discharge plasma catalytic degradation of bisphenol A over graphene/CdS: process parameters optimization and O3 activation mechanism analysis

    2023-11-16 05:38:04NanJIANG姜楠XuechuanLI李學(xué)川JuLI李舉JieLI李杰BingLIAO廖兵BangfaPENG彭邦發(fā)andGuoLIU劉國
    Plasma Science and Technology 2023年10期
    關(guān)鍵詞:李杰

    Nan JIANG(姜楠),Xuechuan LI(李學(xué)川),Ju LI(李舉),Jie LI(李杰),2,?,Bing LIAO (廖兵), Bangfa PENG (彭邦發(fā)) and Guo LIU (劉國)

    1 School of Electrical Engineering,Dalian University of Technology,Dalian 116024,People’s Republic of China

    2 Key Laboratory of Industrial Ecology and Environmental Engineering,University of Technology,Dalian 116024, People’s Republic of China

    3State Environmental Protection Key Laboratory of Synergetic Control and Joint Remediation for Soil &Water Pollution, Chengdu University of Technology, Chengdu 610059, People’s Republic of China

    Abstract

    Keywords: pulsed discharge, gas-liquid discharge, wastewater treatment, parameters optimization, DFT calculation

    1.Introduction

    Bisphenol A(BPA)is an organic raw material widely used to synthesize chemical products such as epoxy resin,polycarbonate, pesticides, antioxidants and coatings, but it is also an emerging contaminant [1].BPA can be discharged into the environment by means of several different channels,including wastewater produced during industrial papermaking, plastics, as well as from landfill leachates [2].When the human body ingests BPA, it will interfere with hormone activities, causing endocrine disorders, and thus endangering human health.Recently, advanced oxidation processes have been established for contaminant degradation by strong oxidization, including photocatalytic degradation [3-6], electrocatalytic degradation [7], Fenton and photo-Fenton-like oxidation [8], ozone oxidation [9] and non-thermal plasma degradation [10, 11].

    Among the above techniques,pulsed discharge plasma is particularly promising on account of its environmentally friendly properties,including generation in the gas phase[12],liquid phase [13] or gas-liquid hybrid phase [14].It is generally believed that a discharge is more easily generated in the gas phase or gas-liquid phase than the liquid phase.During pulsed discharge plasma processes,a mass of reactive oxygen species (ROS) can be generated in situ in liquid and gasliquid environments, such as O3, H2O2, ·OH, ·O, etc, which can uniformly disperse in solution and degrade the organic contaminants.Hydroxyl radical(·OH) is of special concern among the ROS, because the oxidation potential of ·OH is 2.80 V and which is capable of oxidizing a broad range of contaminants non-selectively [15].Simultaneously, physical effects such as ultraviolet light concomitantly produced in a gas-liquid discharge can also improve the efficiency of contaminant degradation.

    The amount of O3generated during discharge is greater than that of ·OH, but the oxidizing capacity of O3is much lower than that of ·OH [16].Therefore, it is critical to boost the conversion of O3to ·OH.The most promising way to promote the O3conversion reaction is to introduce a catalyst.Different catalysts have been designed and employed to promote the conversion of O3either in the gas or liquid phase[17, 18].As a kind of n-type semiconductor photocatalyst,CdS has the unique advantage of various crystallite phases to enhance activity, a narrow band gap (2.42 eV) to achieve‘pseudo photocatalysis’ and a suitable band structure for the reduction of O2/O3to·O-2/·O-3[19-23].However,pure CdS has several problems such as a high charge recombination rate,serious photocorrosion,and the photogenerated holes are prone to oxidize sulfide ions in CdS, resulting in poor stabilityand lowphotocatalytic activity [24-26].Therefore, the photocorrosion and photocatalytic activity of CdScan be improved by doping two-dimensional planar monoatomic layer graphene oxide (GO) with a high specific surface area and carrier mobility.In previous work, we have explored the combination of plasma and a series of reduced GO-CdS(rGO(x)/CdS)catalysts to degrade BPA.Similar to the behavior of photocatalysts in producing ROS,the‘pseudo photocatalytic’effect of catalysts can be induced by the discharge and the production of ·OH enhanced [27-29].Generally speaking,ozonation of contaminants can proceed in two ways: (1) the direct reaction of O3molecules and(2) the indirect oxidation of ·OH resulting from the decomposition of O3.However, to the best of our knowledge, there are few literature reports regarding the mechanism of O3activation to ·OH on the catalyst surface.

    The present study primarily focused on optimizingthe effects of a series of process parameters on the efficacy of pulsed gas-liquid discharge plasma for BPA degradation,including pulse peak voltage, air flow rate, electrode gap,catalyst dosage, initial BPA concentration, initial solution pH,and solution conductivity.Furthermore, the short-lived active species generated during the pulsed gas-liquid plasma discharge was diagnosed by optical emission spectroscopy(OES).Finally, the activation mechanism of O3on the catalyst surface was analyzed using density functional theory (DFT).

    2.Experiment

    2.1.Materials

    The following chemicals have been used in this work: BPA,GO, cadmium acetate, dimethyl sulfoxide (DMSO), (3-aminopropyl)triethoxysilane,acetone and ethanol.All reagents in this work were of analytical grade and purchased from Dalian Liaodong Chemical Reagent Factory, China.The solutions used in the experiment were all prepared with deionized water.

    2.2.Synthesis of rGO/CdS catalysts

    The GO/CdS nanoparticles were synthesized by a hydrothermal method.The synthesis procedure is as follows.First,rGO was fabricated by the Hummers method [30], and then different weight ratios of rGO with Cd(AC)2·2(H2O) were dispersed into DMSO solution to obtain respective contents of 0%,1%,5%,9%and 13%rGO nanocomposites,represented as CdS and rGO(x)/CdS (x=1, 5, 9, 13), respectively.The preparation process of the rGO(x)/CdS catalyst is described in detail in the Supplementary Information.As described in our previous work [27], the highest BPA degradation efficiency was achieved over rGO(5)/CdS catalyst.Therefore,the experiments in this work were carried out over rGO(5)/CdS catalyst.

    2.3.Experimental setup

    The pulsed gas-liquid hybrid discharge plasma (PHDP) for BPA degradation was ignited in a multi-needle to plate electrode,as shown in figure 1.0.10-0.30 g l-1rGO(5)/CdS nanocomposites were added into wastewater for BPA degradation.The initial concentration of BPA varies from 20 to 80 mg l-1and the solution volume for each experiment was 150 ml.The pH values of solution were adjusted to acidic(pH=3, 6), neutral (pH=7.5) and alkaline (pH=9) for the study,and the solution conductivities were 10,50,75 and 100 μS m-1, respectively.The high-voltage electrode consisted of several needles with a 4:1 length to diameter ratio.A steel plate with a 1:3 thickness to diameter ratio served as the ground electrode.The distances between the high-voltage electrode and the ground electrode were 8, 10, and 12 mm.The electric characteristics were measured by a voltage probe,a current monitor, and an oscilloscope.The voltage and current waveforms during the discharge process are demonstrated in figure S1.The gas is pumped into the aeration tank through an air pump and a flowmeter, and then enters the solution tank via the hollow needle electrode to excite the pulsed gas-liquid hybrid discharge plasma.The optical emission spectra (OES) emitted from the pulsed gas-liquid discharge plasma were identified by a spectroscopy (Princeton,Action SP2750).The BPA concentration was determined by high-performance liquid chromatography.The methods for calculation of BPA degradation efficiency and the detection of active species are provided in the Supplementary Information.

    Figure 1.Diagram of the experimental system.

    3.Results and discussion

    3.1.Optimization of process parameters of the pulsed gasliquid discharge plasma catalysis system

    3.1.1.Effect of pulse peak voltage.Contaminant degradation

    is affected by the generation rate and quantity of energetic electrons,active species and UV,which are related to the input voltage [31].Generally, a higher peak discharge voltage will produce more high-energy electrons, thereby accelerating the formation of active species.Hence, the effect of the pulse voltage on the catalytic degradation of BPA by the plasma synergistic rGO(5)/CdS catalyst was first investigated(figure 2(a)).The degradation of 20 mg l-1BPA solution was conducted at three pulse peak voltages(15,17 and 19 kV).

    Notably, BPA degradation was an increasing function of processing time regardless of the pulse peak voltage applied to the reaction system.It is clear from figure 2(a) that the percentage degradation efficiency of BPA is promoted by increasing the discharge peak voltage, and better degradation performance can be achieved at a higher peak voltage.For target concentrations<1.0 mM, the reaction rate is proportional to the initial concentration based on the Langmuir-Hinshelwood model [32, 33].Hence, the first-order rate constants(r=-dc/dt=kKC=k1C or ln C0/Ct=k1t)were calculated and are displayed in figure 2(b).When the peak voltages were 15,17 and 19 kV,the kinetic constants reached 0.016,0.025 and 0.037 min-1,respectively.That is because the number of active species will increase as the voltage increases.The increase in active species can increase the probability of collision with contaminant molecules, which will resultin higher BPA degradation.Meanwhile, the intensity of the electric field and ultraviolet light generated in the reactor will also increase[34-36].Guo et al[37]studied BPA degradation in aqueous solution by plasma combined with activated carbon under different voltages and came to similar conclusions.Considering various factors comprehensively, 19 kV was selected as the discharge voltage in subsequent experiments.

    Figure 2.(a)Effect of pulse peak voltage on BPA degradation and(b)kinetic curves of BPA degradation(BPA concentration=20 mg l-1,air flow rate=4 l min-1, electrode gap=10 mm, catalyst dosage=0.2 g l-1, pH value=7.5, solution conductivity=10 mS cm-1).

    Figure 3.(a) Effect of air flow rate on BPA degradation and (b)kinetic curves of BPA degradation(BPA concentration=20 mg l-1,pulse peak voltage=19 kV, electrode gap=10 mm, catalyst dosage=0.2 g l-1, pH value=7.5, solution conductivity=10 mS cm-1).

    3.1.2.Effect of air flow rate.The air flow rate can significantly affect the physical and chemical effects in plasma system,such as the number of active species.When air is pumped into the system during the discharge process, many active species including O·, O3, ·OH, H·, N·, etc can be generated in the reaction system.Figure 3(a)shows the effect of air flow rate on BPA degradation.It can be seen from figure 3(a) that BPA degradation efficiency increases first and then decreases as the air flow rate increases from 2 to 6 l min-1.The highest degradation efficiency was achieved when the air flow rate was 4 l min-1.That is because the number of oxygen molecules increases with the air flow rate, which increases the O3concentration.Zhang et al[38]reported that an increase in air flow rate favored the transfer of O3from the gas phase to the liquid phase.In addition,the residence time of active species in the reactor can also be affected by the air flow rate.As the air flow rate increases, the residence time of active substances in the solution will be shortened, and thus the active particles cannot effectively dissolveinto the solution and participate in the degradation of organic pollutants[39].In contrast,a higher air flow rate will cause a large number of fine bubbles to merge into coarse bubbles,which will destroy the transfer balance and lead to a reduction in the gas-liquid mass transfer of active species [40].In addition, as shown in figure 3(b), it can be concluded that the highest kinetic constant (0.036 min-1) can be obtained when the air flow rate is 4 l min-1.

    Figure 4.(a) Effect of electrode gap on BPA degradation and (b)kinetic curves of BPA degradation(BPA concentration=20 mg l-1,pulse peak voltage=19 kV, air flow rate=4 l min-1, catalyst dosage=0.2 g l-1, pH value=7.5, solution conductivity=10 mS cm-1).

    3.1.3.Effect of electrode gap.In a discharge plasma system,the discharge mode will alter with the change in the electrode gap,which will affect the production of active species as well as the degradation performance.Figure 4(a) shows the effect of electrode gap on BPA degradation.As shown in figure 4(a), the BPA degradation efficiency increases as the electrode gap increases from 8 to 10 mm.With further increase in the electrode gap to 12 mm,the BPA degradation efficiency decreases.Generally speaking, the electric field is enhanced with a decrease in the electrode gap, which facilitates the formation of reactive species.Nevertheless,when the discharge gap is further reduced to 8 mm, the discharge mode transforms into an unstable spark discharge.Zhan et al [41, 42] also reported that the discharge mode transferred from a corona discharge to a spark discharge when the electrode gap was decreased, which resulted in a rapid decrease in voltage and an increase in current.Furthermore,the kinetic analysis also demonstrates that the maximum kinetic constant can be acquired with an electrode gap of 10 mm (figure 4(b)).Therefore, the optimal electrode gap is 10 mm.

    Figure 5.(a) Effect of catalyst dosage on BPA degradation.and (b)pseudo-first-order kinetic curves of BPA degradation (BPA concentration=20 mg l-1, pulse peak voltage=19 kV, air flow rate=4 l min-1,electrode gap=10 mm,pH value=7.5,solution conductivity=10 mS cm-1).

    3.1.4.Effect of catalyst dosage.The effect of rGO(5)/CdS catalyst dosage on BPA degradation efficiency was studied.As exhibited in figure 5(a), as the dosage of rGO(5)/CdS catalyst increased from 0.1 to 0.3 g l-1, the degradation efficiency first increased and then decreased.The highest degradation efficiency was achieved at 0.2 g l-1.A significant inhibitory effect appeared whenthe catalyst dosage continued to increase.We speculated that when the dosage of rGO(5)/CdS is increased within a certain range,the plasma can activate ‘pseudo photocatalytic’ behavior of the catalyst and generate more photogenerated e--h+pairs,which is conducive to the production of ·OH, thereby improving the degradation BPA.However,adding too much catalyst not only leads to a higher cost but also reduces the number of reactive active sites due to the aggregation of solid particles, which is not conducive to contaminant degradation [43, 44].Figure 5(b) displays the effect of catalyst dosage on the kinetic constants.It can be seen from figure 5(b) that the pseudo-first-order kinetic curve and the kinetic constants are consistent with those of the catalyst dosage.Therefore, the addition of 0.2 g l-1of catalyst was considered to be the optimal dosage for BPA elimination in this work.

    Figure 6.(a)Effect of initial concentration on BPA degradation and(b)kinetic curves of BPA degradation(pulse peak voltage=19 kV,air flow rate=4 l min-1, electrode gap=10 mm, catalyst dosage=0.2 g l-1, pH value=7.5, solution conductivity=10 mS cm-1).

    3.1.5.Effect of initial concentration of BPA.Figure 6(a)

    exhibits the evolution of BPA degradation efficiency over time at different initial BPA concentrations.It is obvious that BPA degradation efficiency and initial concentration demonstrate a negative correlation.Nezamzadeh-Ejhieh pointed out that increasing the number of molecules per unit volume helps to increase the probability of collision with active particles, which is conducive to improving the degradation efficiency [45, 46].However, we found that the reactive speciesis not enough to react with contaminants,resulting in a lower BPA degradation efficiency at the same time[47].More time was needed for a higher concentration of BPA.Nevertheless, a higher degradation rate does not mean that more contaminants are decomposed.With initial concentrations of 20, 50 and 80 mg l-1, the absolute mass of BPA removed was 2.63 mg, 5.55 mg and 7.27 mg respectively.The absolute mass of BPA removed showed an opposite trend to degradation efficiency.The main reason for this phenomenon was that the collision probability between active species and BPA molecules was greatly increased.The higher initial concentration means that there is intense competition between reactant molecules for reactive species.Correspondingly, a maximum kinetic constant of about 0.036 min-1can be achieved at 20 mg l-1, which is 1.6 and 2.3 times that for the 50 mg l-1and 80 mg l-1solutions(see figure 6(b)).

    Figure 7.(a)Effect of initial solution pH on BPA degradation,(b)kinetic curves of BPA degradation and(c)effect of pH on zeta potential(BPA concentration=20 mg l-1, pulse peak voltage=19 kV, air flow rate=4 l min-1, electrode gap=10 mm, catalyst dosage=0.2 g l-1,solution conductivity=10 mS cm-1).

    3.1.6.Effect of initial solution pH.The initial solution pH can affect the number of active substances and the species of the organic compounds during the discharge plasma process[48].There are two plausible reasons to analyze the effect of pH on the degradation of any organic compound: (1) pH affects the availability of reactive species and (2) pH affects the organic compound, which undergoes structural variations [49].It has been reported that the structure of organic compounds changes due to protonation and deprotonation with variations in solution pH [50-52].Hence, it is vital to evaluate the effect of pH on BPA degradation by changing the solution pH between 3 and 9.

    The BPA degradation efficiency and reaction rate constant as a function of initial concentration are presented in figures 7(a) and (b).It can be clearly observed from figure 7(a) that a higher BPA degradation efficiency was acquired under neutral conditions(initial pH 7.5),followed by alkaline and weak acidic conditions.Meanwhile, kinetic constants also follow the same rule.This can be attributed to the fact that BPA is present in molecular form in aqueous solution when the initial solution pH is lower than the BPA dissociation constant (4.9).Conversely, BPA is present as in anion form at pH levels higher than 4.9 [53].It has been reported that pollutants in anion form are react more easily with ROS produced from plasma [53, 54].Secondly, H+in the acidic solution will consume many electrons,which is not conducive to the formation of the active species ·OH [55].

    In addition, zeta potentials in different pH solutions were measured, as displayed in figure 7(c).Zeta potential is used to analyze the charge of rGO(5)/CdS catalyst.As shown in figure 7(c),the zeta potential of rGO(5)/CdS decreases with the increase of pH.The zeta potential was located between pH 9-10(~9.7),which is characterized as the point of zero charge(PZC).When the pH value of the solution is less than PZC,the catalyst surface is positively charged, while when the pH value of the solution is greater than PZC, the catalyst surface is negatively charged [56, 57].Hence, there is non-interaction between rGO(5)/CdS and BPA at pH<4.9.As pH begins to increase(4.99.7, the negatively charged catalyst repels BPA anion and the degradation efficiency tends to decrease.Furthermore,Ren et al[58]reported that the surface of CoOOH was protonated or deprotonated when solution pH was lower or higher than its PZC.At PZC 3.1,the surface of CoOOH was mostly zero charged, and the trans-ferulic acid degradation became the maximum.However, the experimental results indicate that the highest removal effect is achieved under neutral conditions.This is because OH-will annihilate the·OH free radicals generated during the discharge process in alkaline environment [59], and then the BPA degradation would be restrained.Herein, the initial solution pH is controlled as 7.5 in the following experiment.

    3.1.7.Effect of solution conductivity.Solution conductivity may affect the discharge characteristic as well as the generation of active species.Hence,it is essential to explore the effect of solution conductivity on BPA degradation in the plasma catalysis process.The effect of solution conductivity on BPA degradation efficiency is presented in figure 8(a).It is clear that the greater the solution conductivity, the worse the removal efficiency of BPA solution.That is because higher conductivity will be accompanied by more intensive UV light and higher plasma temperature, which may have a negative effect on reactive species production [50, 60].Correspondingly, the kinetic constant also decreases from 0.035 to 0.014 min-1when increasing the solution conductivity from 10 to 100 μS m-1, as shown in figure 8(b).Therefore, the following experiment was carried out at the initial conductivity of 10 mS cm-1.

    3.2.The identification of reactive species and analysis of their contribution

    Figure 8.(a) Effect of solution conductivity on BPA degradation and (b) kinetic curves of BPA degradation (BPA concentration=20 mg l-1,pulse peak voltage=19 kV,air flow rate=4 l min-1,electrode gap=10 mm, catalyst dosage=0.2 g l-1,pH value=7.5).

    Figure 9.OES of the air gas-liquid hybrid discharge plasma (pulse peak voltage=19 kV, frequency=50 Hz, air flow rate=4 l min-1, electrode gap=10 mm).

    3.2.1.Optical emission spectra diagnosis.As is well known,·OH is a vital oxidant that dominates plasma oxidations in water treatment, and ·O plays an important role in the formation of O3.Hence,the OES ranging from 200 to 850 nm were diagnosed to investigate the types of reactive species generated (including ·O and ·OH) in the pulsed gas-liquid plasma system,as shown in figure 9.The results show that the peaks located in the short-wave region belong to the spectrum of OH·emission, which is mainly the energy transition A2Σ+→X2П.The peaks in visible range are the emission line of the hydrogen atom H(n=3,4,5)→H(n=2).The Balmer spectrum of H corresponds to Hα(656.3 nm), Hβ(486.1 nm)and Hγ(434.0 nm),respectively.The peaks in the infrared range belong to the spectrum of the oxygen atom O,corresponding to the energy state transitions of O 3p5P0→3s5S0(777.1 nm) and 3p3P→3s3S0(844.6 nm),respectively.As in the air gas-liquid discharge, the active oxygen atoms are preferentially generated from O2.The formation of active species can be explained by equations (1)-(8) [14, 61]:

    3.2.2.The contribution of reactive species to BPA degradation.The contribution of various chemically reactive species to BPA degradation and plasma catalytic processes over the catalyst was investigated by the free radical capture test(figure 10).Benzoquinone (BQ), monopotassium phosphate(MP),iso-propyl alcohol(IPA)and sodium oxalate(SO) were acted as ·O2-(k=2×109M-1s-1), e-(k=1.9×107M-1s-1), ·OH (k=1.9×1010M-1s-1)and h+(k>4.7×107M-1s-1) scavengers, respectively[62-65].The plasma treatment time was 60 min.As presented in figure 10, after adding MP and SO, the degradation efficiency was reduced by about 41.4% and 53.6%,respectively, which was 1.39 and 2.16 times that of the plasma alone.These results indicate that e-and photogenerated h+play an important role in BPA degradation.In our previous work, the ‘pseudo photocatalytic’ mechanism of plasma-induced rGO(5)/CdS catalysts was elucidated.These results show that the adsorption range of visible light is widened and the separation of e--h+pairs is accelerated when rGO is added to CdS [27].

    In the case of plasma alone, the presence of BQ had almost no effect on BPA degradation (0.62%).However, the removal rate was decreased by 28.8% after introducing BQ,indicating that the derived reactive species produced byplay an important role in reaction process.In a plasma catalytic system,can also be converted to-to participate in the BPA degradation reaction.Moreover, after the addition of IPA, the BPA degradation efficiency is also reduced to a certain extent, indicating that the presence of·OH in the reaction system would also have an impact on BPA degradation.

    Figure 10.The capture testing of active species in PHDP and PHDP catalytic systems at 60 min.

    3.3.O3 activation mechanism analysis

    As a long-lived species, O3can diffuse into the liquid phase and react with aqueous contaminants in air or oxygen discharge.At the gas-liquid interface, strongly oxidative compounds such as ·OH radicals and O atoms can be generated and dissolved in water,and organic pollutants can be removed through a series of oxidation reactions [66].Variations in the concentrations of O3and ·OH in PHDP and PHDP catalytic systems at different treatment times (30 min and 60 min) are exhibited in figure S3.As can be seen from that figure, the presence of rGO(5)/CdS catalyst reduces the O3concentration in the PHDP system and promotes the generation of·OH,which facilitates BPA degradation.Some of dominant reactions for O3and ·OH production are presented in equations (9)-(13) [66-68]:

    There are few studies on the mechanism of how O3is activated and converted to ·OH on the catalyst surface gasliquid discharge.Therefore, it is also necessary to study the evolution process of active species in the plasma catalytic system,especially the activation of O3on the surface of rGO(5)/CdS nanocomposite catalyst.The activation pathway of O3on the catalyst surface was therefore analyzed in detail by DFT.The method of theoretical simulation is described in text S4.

    Figure 11.(a) The O3 activation pathway on the rGO(5)/CdS surface and (b)the corresponding energy profile.In free O3 and O2,the O-O bonds have lengths of 1.31 ? and 1.27 ?, respectively.

    Based on DFT calculations, the activation path of O3adsorbed on the surface of rGO(5)/CdS is exhibited in figure 11.First,O3binds to the C atom in rGO(figure 11(a)).The adsorption energy of this interaction is 0.72 eV, which effectively weakens the O1-O2bond with a length of 1.98 ?(figure 11(b)), indicating that O3adsorbed on the surface of rGO(5)/CdS is activated.Meanwhile,the O2-O3bond with a length of 1.28 ? is enhanced,which means that O2-O3can be desorbed into free O2with a desorption energy of 0.04 eV(figure 11(b)).Subsequently, an O1atom binds to H2O to form adsorbed ·OH.Finally, ·OH is desorbed, and this step determines the rate of the reaction, for which the energy barrier is 1.82 eV.

    The projected density of states(PDOS)of O atoms in O3further confirms the activation mechanism of O3,as shown in figure 12(a).After the adsorption of O3on the rGO(5)/CdS surface,the 2p state of the O1atom is located below the Fermi level, indicating that electrons are clustered in the O1atom.However, some 2p states of O2and O3atoms are above the Fermi level and not occupied by electrons.Therefore, the above results indicate that the electrons in rGO(5)/CdS are mainly concentrated in the O1atom, which is directly bound to the C atom.This is further illustrated by the charge density difference mapping of O3and rGO(5)/CdS (figure 12(b)).The sky blue and yellow isosurfaces represent negative and positive charges,respectively.The charge density isosurfaces in all figures are set as 0.002 e ?-3.The calculated results show that the electrons in rGO(5)/CdS (sky blue region) are mainly located between O1atoms and rGO,which proves that O3is activated.

    Figure 12.(a)The calculated projected density of state plots of O3 on rGO(5)/CdS and(b)the charge density difference mapping between O3 and rGO(5)/CdS.

    4.Conclusions

    Evaluation and optimization of the PHDP system over rGO(5)/CdS were performed in terms of BPA degradation performance in aqueous solution.The results indicated that increasing discharge voltage and decreasing initial BPA concentration and solution conductivity were found to be favorable for BPA degradation.With the increase of other process parameters (air flow rate, electrode gap, catalyst dosage and initial solution pH), the BPA degradation rate increased first and then decreased.The short-lived and longlived activespecies generated from pulsed gas-liquid hybrid discharge plasma were detected by optical emission spectroscopy, and their contribution to BPA degradation was evaluated by the free radical capture test.Finally, DFT calculation was used to analyze the activation mechanism of O3on the catalyst surface.The O3adsorbed on the surface of rGO(5)/CdS is activated and desorbed into free O2, and the step of desorption to ·OH is the rate-determining step of the reaction.The projected density of states of O atoms in O3further confirmed the activation mechanism of O3.

    Acknowledgments

    This work is supported by the Open Fund for State Environmental Protection Key Laboratory of Synergetic Control and Joint Remediation for Soil & Water Pollution (No.GHBK-2020-006) and National Natural Science Foundation of China (No.21876070).

    猜你喜歡
    李杰
    Memristor’s characteristics: From non-ideal to ideal
    A spintronic memristive circuit on the optimized RBF-MLP neural network
    基于SPSS軟件建立ARIMA模型
    客聯(lián)(2022年3期)2022-05-31 04:28:08
    Effect of megapore particles packing on dielectric barrier discharge, O3 generation and benzene degradation
    Multi-band asymmetric transmissions based on bi-layer windmill-shaped metamaterial*
    人民海軍首次海戰(zhàn)
    源流(2021年11期)2021-03-25 10:32:07
    小胖熊半夜歷險記
    Zero-Sequence Current Suppression Strategy for Open-End Winding Permanent Magnet Synchronous Motor Based on Model Predictive Control
    ?。楱#镅酲耍颞Γ?多duō 多duo
    Numerical investigation of the time-resolved bubble cluster dynamics by using the interface capturing method of multiphase flow approach*
    99热这里只有是精品50| 免费搜索国产男女视频| 国产精品国产三级国产av玫瑰| 色哟哟·www| 哪里可以看免费的av片| 禁无遮挡网站| 亚洲欧美精品综合久久99| 小蜜桃在线观看免费完整版高清| 国内精品美女久久久久久| 久久精品久久久久久噜噜老黄 | 国产精品av视频在线免费观看| 日日撸夜夜添| 色播亚洲综合网| 最新在线观看一区二区三区| 亚洲欧美成人精品一区二区| 国产男靠女视频免费网站| 日本精品一区二区三区蜜桃| 男人和女人高潮做爰伦理| 中文在线观看免费www的网站| 一个人看的www免费观看视频| 一级a爱片免费观看的视频| 乱人视频在线观看| 成人鲁丝片一二三区免费| 午夜免费男女啪啪视频观看 | 久久久久性生活片| 国产亚洲精品综合一区在线观看| 国产av在哪里看| 97在线视频观看| 亚洲国产色片| 赤兔流量卡办理| 国产高潮美女av| 亚洲18禁久久av| 亚洲欧美清纯卡通| 大又大粗又爽又黄少妇毛片口| 国产亚洲精品久久久久久毛片| 男女做爰动态图高潮gif福利片| 日本a在线网址| 欧美丝袜亚洲另类| 一个人看视频在线观看www免费| 久久热精品热| 久久久精品欧美日韩精品| 非洲黑人性xxxx精品又粗又长| 天堂av国产一区二区熟女人妻| 亚洲欧美精品自产自拍| 丰满人妻一区二区三区视频av| 午夜老司机福利剧场| 亚洲第一电影网av| 国产伦在线观看视频一区| 午夜福利在线观看免费完整高清在 | 亚洲人成网站在线观看播放| 国产欧美日韩精品亚洲av| 免费黄网站久久成人精品| 欧美另类亚洲清纯唯美| 国产在线精品亚洲第一网站| 亚洲不卡免费看| 中出人妻视频一区二区| 秋霞在线观看毛片| 男人狂女人下面高潮的视频| 国产真实乱freesex| 丝袜美腿在线中文| 激情 狠狠 欧美| 国产精品人妻久久久影院| 亚洲美女视频黄频| 天堂动漫精品| 噜噜噜噜噜久久久久久91| 一个人观看的视频www高清免费观看| 1024手机看黄色片| 啦啦啦啦在线视频资源| 国产又黄又爽又无遮挡在线| 男女那种视频在线观看| 一级黄色大片毛片| 国产伦精品一区二区三区视频9| 卡戴珊不雅视频在线播放| 欧美日韩精品成人综合77777| 少妇的逼好多水| 国产人妻一区二区三区在| 可以在线观看毛片的网站| 国产女主播在线喷水免费视频网站 | 国产高清有码在线观看视频| 亚洲图色成人| 国产女主播在线喷水免费视频网站 | 午夜福利成人在线免费观看| 在线天堂最新版资源| 我的女老师完整版在线观看| 能在线免费观看的黄片| 亚洲无线观看免费| 日本 av在线| 日韩欧美精品免费久久| 麻豆一二三区av精品| 日韩精品青青久久久久久| 激情 狠狠 欧美| 久久人人爽人人片av| av黄色大香蕉| 嫩草影院新地址| 国产精品一区二区三区四区免费观看 | 中文亚洲av片在线观看爽| 婷婷精品国产亚洲av在线| 久久中文看片网| 丝袜美腿在线中文| 麻豆精品久久久久久蜜桃| 老司机福利观看| 国产精品人妻久久久久久| av在线蜜桃| 日本 av在线| av在线天堂中文字幕| 欧美成人精品欧美一级黄| 欧美激情久久久久久爽电影| 国产成人91sexporn| 国产亚洲精品久久久com| 亚洲欧美日韩高清在线视频| 村上凉子中文字幕在线| 九色成人免费人妻av| 亚洲成人久久爱视频| 欧美高清成人免费视频www| 欧美日本亚洲视频在线播放| 搡老妇女老女人老熟妇| 日本撒尿小便嘘嘘汇集6| 免费一级毛片在线播放高清视频| 免费av毛片视频| 日韩欧美三级三区| 久久久久久伊人网av| 在线免费观看的www视频| 亚洲最大成人手机在线| 又爽又黄无遮挡网站| 真人做人爱边吃奶动态| 我的老师免费观看完整版| 日日撸夜夜添| 插阴视频在线观看视频| 99久国产av精品国产电影| 日本三级黄在线观看| 午夜视频国产福利| 日本-黄色视频高清免费观看| 两个人的视频大全免费| 少妇丰满av| 免费看美女性在线毛片视频| 男人的好看免费观看在线视频| 男人狂女人下面高潮的视频| 亚洲av不卡在线观看| 深夜精品福利| 97热精品久久久久久| 欧美中文日本在线观看视频| 联通29元200g的流量卡| 插逼视频在线观看| 成人三级黄色视频| 久久精品人妻少妇| 偷拍熟女少妇极品色| 欧美极品一区二区三区四区| 在线国产一区二区在线| 欧美+日韩+精品| 99久久久亚洲精品蜜臀av| 久久精品国产亚洲av香蕉五月| 久久亚洲精品不卡| 免费人成在线观看视频色| av福利片在线观看| 国内精品美女久久久久久| 一进一出好大好爽视频| 亚洲精品久久国产高清桃花| 好男人在线观看高清免费视频| 成人美女网站在线观看视频| 精品熟女少妇av免费看| 国产不卡一卡二| 九九热线精品视视频播放| 欧美一区二区亚洲| 97超视频在线观看视频| 国产精品三级大全| 嫩草影院新地址| 91精品国产九色| 日韩成人伦理影院| 国产精品亚洲美女久久久| 少妇人妻一区二区三区视频| 91麻豆精品激情在线观看国产| 18禁裸乳无遮挡免费网站照片| 日本在线视频免费播放| 91狼人影院| 天天一区二区日本电影三级| 国内少妇人妻偷人精品xxx网站| 亚洲精品成人久久久久久| av在线天堂中文字幕| 乱人视频在线观看| 美女 人体艺术 gogo| 亚洲丝袜综合中文字幕| 变态另类成人亚洲欧美熟女| 国产精品久久久久久精品电影| 国产男人的电影天堂91| 久久精品国产99精品国产亚洲性色| 女同久久另类99精品国产91| 美女xxoo啪啪120秒动态图| 国产精品美女特级片免费视频播放器| 亚洲va在线va天堂va国产| 少妇人妻精品综合一区二区 | 日韩欧美精品免费久久| 老师上课跳d突然被开到最大视频| 变态另类成人亚洲欧美熟女| www.色视频.com| 国产精品爽爽va在线观看网站| 少妇高潮的动态图| 色哟哟哟哟哟哟| 九九久久精品国产亚洲av麻豆| 国产精品国产三级国产av玫瑰| av天堂在线播放| 欧美一区二区国产精品久久精品| 国产片特级美女逼逼视频| 国内精品久久久久精免费| 91午夜精品亚洲一区二区三区| 国产欧美日韩精品亚洲av| 亚洲精品影视一区二区三区av| 日本黄色片子视频| 久久久久国产精品人妻aⅴ院| 一区二区三区高清视频在线| 人人妻人人澡欧美一区二区| 亚洲性夜色夜夜综合| 中文字幕精品亚洲无线码一区| 午夜免费男女啪啪视频观看 | 九九热线精品视视频播放| 美女免费视频网站| 国产男人的电影天堂91| 亚洲av免费高清在线观看| 色尼玛亚洲综合影院| 日韩一区二区视频免费看| 亚洲不卡免费看| 国产伦一二天堂av在线观看| 亚洲中文字幕日韩| 床上黄色一级片| 国产成人aa在线观看| 国产成人一区二区在线| 五月伊人婷婷丁香| 性色avwww在线观看| 国产精品电影一区二区三区| 12—13女人毛片做爰片一| 长腿黑丝高跟| 最近的中文字幕免费完整| 亚洲精华国产精华液的使用体验 | 成年女人看的毛片在线观看| 九九热线精品视视频播放| av女优亚洲男人天堂| 两性午夜刺激爽爽歪歪视频在线观看| 免费电影在线观看免费观看| 能在线免费观看的黄片| 中国美白少妇内射xxxbb| 国产 一区精品| 99riav亚洲国产免费| 国产伦精品一区二区三区四那| 最好的美女福利视频网| 91久久精品国产一区二区成人| av黄色大香蕉| 免费在线观看影片大全网站| a级毛片a级免费在线| 精品日产1卡2卡| av福利片在线观看| 亚洲熟妇中文字幕五十中出| 给我免费播放毛片高清在线观看| 真实男女啪啪啪动态图| 国产精品综合久久久久久久免费| 变态另类丝袜制服| 国产69精品久久久久777片| .国产精品久久| 国产黄a三级三级三级人| 亚洲国产色片| 午夜视频国产福利| 午夜福利18| 免费人成视频x8x8入口观看| 99热这里只有精品一区| 国产白丝娇喘喷水9色精品| 欧美日韩精品成人综合77777| 最近中文字幕高清免费大全6| 中文字幕免费在线视频6| 国产精品一区二区三区四区免费观看 | 亚洲精品在线观看二区| 久久久国产成人免费| 国内精品一区二区在线观看| 少妇裸体淫交视频免费看高清| 成人综合一区亚洲| 免费不卡的大黄色大毛片视频在线观看 | 12—13女人毛片做爰片一| 六月丁香七月| 少妇熟女aⅴ在线视频| a级毛片免费高清观看在线播放| 国产综合懂色| 菩萨蛮人人尽说江南好唐韦庄 | 精品免费久久久久久久清纯| 尾随美女入室| 露出奶头的视频| 又黄又爽又刺激的免费视频.| 免费看a级黄色片| 国产真实乱freesex| 国产高清不卡午夜福利| 亚洲高清免费不卡视频| 黄色一级大片看看| 日韩欧美免费精品| 亚洲欧美成人精品一区二区| 哪里可以看免费的av片| 人妻丰满熟妇av一区二区三区| 久久这里只有精品中国| 成年av动漫网址| 2021天堂中文幕一二区在线观| 亚洲欧美日韩高清专用| 国内精品美女久久久久久| 午夜福利在线观看吧| 久久精品国产亚洲av涩爱 | 97超级碰碰碰精品色视频在线观看| 九九在线视频观看精品| 18禁裸乳无遮挡免费网站照片| 黄色一级大片看看| 欧美一区二区亚洲| 中文资源天堂在线| 噜噜噜噜噜久久久久久91| 精品久久久噜噜| 99久久精品热视频| 亚洲第一电影网av| 午夜a级毛片| 欧美3d第一页| 99国产极品粉嫩在线观看| 久99久视频精品免费| 亚洲电影在线观看av| 国产精品久久久久久av不卡| 看十八女毛片水多多多| 床上黄色一级片| 干丝袜人妻中文字幕| 春色校园在线视频观看| 能在线免费观看的黄片| 日本精品一区二区三区蜜桃| 18禁在线无遮挡免费观看视频 | 亚洲人成网站在线播放欧美日韩| 亚洲国产欧洲综合997久久,| 悠悠久久av| 免费看a级黄色片| 舔av片在线| 午夜精品国产一区二区电影 | 男插女下体视频免费在线播放| 欧美潮喷喷水| 亚洲欧美日韩无卡精品| videossex国产| 美女被艹到高潮喷水动态| 午夜福利18| 午夜老司机福利剧场| 免费人成在线观看视频色| 色在线成人网| 岛国在线免费视频观看| 国产综合懂色| av天堂在线播放| 午夜福利视频1000在线观看| 亚洲人成网站在线观看播放| 午夜a级毛片| 亚洲国产精品成人久久小说 | 小说图片视频综合网站| 国产精品福利在线免费观看| 一个人观看的视频www高清免费观看| 日日摸夜夜添夜夜添av毛片| 亚洲内射少妇av| 久久草成人影院| 夜夜看夜夜爽夜夜摸| 亚洲性夜色夜夜综合| 97人妻精品一区二区三区麻豆| 日韩强制内射视频| 校园春色视频在线观看| 丝袜喷水一区| 麻豆久久精品国产亚洲av| 听说在线观看完整版免费高清| 在线免费观看不下载黄p国产| 国产伦精品一区二区三区四那| 男女下面进入的视频免费午夜| 在线免费十八禁| 少妇高潮的动态图| 九色成人免费人妻av| 欧美极品一区二区三区四区| 两个人的视频大全免费| 久久久久国内视频| 国产伦在线观看视频一区| 国产成年人精品一区二区| 一本精品99久久精品77| 免费不卡的大黄色大毛片视频在线观看 | 日本成人三级电影网站| 久久九九热精品免费| 亚洲欧美精品自产自拍| 国产真实乱freesex| 国产精品综合久久久久久久免费| 午夜激情欧美在线| 日本五十路高清| 国产成人aa在线观看| 男女啪啪激烈高潮av片| 国产视频内射| 成人三级黄色视频| 成人亚洲精品av一区二区| 日韩欧美精品v在线| 国产69精品久久久久777片| 国产精品无大码| 蜜桃亚洲精品一区二区三区| 搡老岳熟女国产| 如何舔出高潮| 丰满的人妻完整版| 久久久久久久亚洲中文字幕| 女生性感内裤真人,穿戴方法视频| 美女被艹到高潮喷水动态| 97在线视频观看| 午夜日韩欧美国产| 亚洲av第一区精品v没综合| 久久鲁丝午夜福利片| 女人十人毛片免费观看3o分钟| 国内精品一区二区在线观看| 欧美成人一区二区免费高清观看| 国产一级毛片七仙女欲春2| 国产精品嫩草影院av在线观看| 三级国产精品欧美在线观看| 精品人妻熟女av久视频| 国产男靠女视频免费网站| 国产亚洲欧美98| 国产精品无大码| 精品日产1卡2卡| 婷婷六月久久综合丁香| 亚洲在线自拍视频| 亚洲无线在线观看| 精品少妇黑人巨大在线播放 | 亚洲性夜色夜夜综合| 国产成人一区二区在线| 免费搜索国产男女视频| 欧美三级亚洲精品| 久99久视频精品免费| 日产精品乱码卡一卡2卡三| 性欧美人与动物交配| 精品久久久久久久久亚洲| 成年av动漫网址| 我的女老师完整版在线观看| 免费观看精品视频网站| 黄色视频,在线免费观看| 国产亚洲精品综合一区在线观看| 国产黄色小视频在线观看| 白带黄色成豆腐渣| 久久天躁狠狠躁夜夜2o2o| 全区人妻精品视频| 一进一出抽搐动态| 色在线成人网| 久久精品国产鲁丝片午夜精品| 亚洲一级一片aⅴ在线观看| 精品久久久噜噜| 日本a在线网址| 国产麻豆成人av免费视频| 国产在视频线在精品| 97超视频在线观看视频| 亚洲中文日韩欧美视频| 久久久精品欧美日韩精品| 欧美日韩国产亚洲二区| 亚洲婷婷狠狠爱综合网| 国产单亲对白刺激| 伦精品一区二区三区| 国产精品三级大全| 国产在视频线在精品| www日本黄色视频网| 最近的中文字幕免费完整| 国产午夜福利久久久久久| 欧美xxxx黑人xx丫x性爽| 国产伦在线观看视频一区| 草草在线视频免费看| 色哟哟·www| 精品午夜福利视频在线观看一区| 久久欧美精品欧美久久欧美| 亚洲人与动物交配视频| 欧美一区二区精品小视频在线| 禁无遮挡网站| 黄色日韩在线| 中国国产av一级| 联通29元200g的流量卡| 国产精品一及| 日本撒尿小便嘘嘘汇集6| 寂寞人妻少妇视频99o| 美女cb高潮喷水在线观看| 国产高潮美女av| 国产亚洲欧美98| 国产精品av视频在线免费观看| 成人美女网站在线观看视频| 舔av片在线| 精品福利观看| 国产真实乱freesex| 男人舔奶头视频| 亚洲人与动物交配视频| 一进一出抽搐gif免费好疼| 久久中文看片网| 欧美日韩乱码在线| 午夜精品一区二区三区免费看| 久久久久久久久大av| 国产精品久久电影中文字幕| 日韩人妻高清精品专区| 国内精品宾馆在线| 插逼视频在线观看| 欧美成人一区二区免费高清观看| 三级经典国产精品| 免费人成视频x8x8入口观看| 伦理电影大哥的女人| 女人十人毛片免费观看3o分钟| 少妇熟女aⅴ在线视频| 插阴视频在线观看视频| 亚洲精品亚洲一区二区| 亚洲人成网站在线播| 精品午夜福利在线看| 97超碰精品成人国产| 免费人成视频x8x8入口观看| 一区二区三区高清视频在线| 日本撒尿小便嘘嘘汇集6| 久久精品国产亚洲av香蕉五月| 成年女人毛片免费观看观看9| 99热网站在线观看| 免费av观看视频| 夜夜爽天天搞| 成人毛片a级毛片在线播放| 成人鲁丝片一二三区免费| 日韩欧美一区二区三区在线观看| 小蜜桃在线观看免费完整版高清| 卡戴珊不雅视频在线播放| 亚洲一区二区三区色噜噜| 久久久国产成人精品二区| 日日撸夜夜添| 中文资源天堂在线| 99riav亚洲国产免费| 男人舔奶头视频| 亚洲国产精品久久男人天堂| 国产精品日韩av在线免费观看| 国产精品一区二区三区四区免费观看 | 直男gayav资源| 色哟哟·www| 国产精品一区二区三区四区免费观看 | 成人高潮视频无遮挡免费网站| 亚洲欧美清纯卡通| 国产av在哪里看| 午夜久久久久精精品| 九九热线精品视视频播放| 国语自产精品视频在线第100页| 成人性生交大片免费视频hd| 黄片wwwwww| 啦啦啦韩国在线观看视频| 亚洲av第一区精品v没综合| 日本黄大片高清| 一级av片app| 97超视频在线观看视频| 搞女人的毛片| 好男人在线观看高清免费视频| 搡老岳熟女国产| 成人综合一区亚洲| 亚洲aⅴ乱码一区二区在线播放| 国内精品美女久久久久久| 中出人妻视频一区二区| 国产国拍精品亚洲av在线观看| 国产成人freesex在线 | 深夜a级毛片| 99热这里只有是精品50| 日韩欧美免费精品| 免费观看在线日韩| 99久国产av精品| 九色成人免费人妻av| 欧美不卡视频在线免费观看| 国产精品一区www在线观看| 最新中文字幕久久久久| 少妇的逼水好多| 欧美成人a在线观看| 日韩精品青青久久久久久| 尤物成人国产欧美一区二区三区| 成人漫画全彩无遮挡| 国产亚洲精品久久久久久毛片| 欧美丝袜亚洲另类| 两个人的视频大全免费| 亚洲人成网站在线播| a级毛片免费高清观看在线播放| 国产精品1区2区在线观看.| 99热全是精品| 免费电影在线观看免费观看| 特级一级黄色大片| 日韩亚洲欧美综合| 男女下面进入的视频免费午夜| 波多野结衣巨乳人妻| 日韩欧美精品免费久久| 色在线成人网| 99热精品在线国产| 国产成人a∨麻豆精品| 日韩av不卡免费在线播放| 又爽又黄a免费视频| 久久精品综合一区二区三区| 国产老妇女一区| 国产亚洲欧美98| 欧美精品国产亚洲| 99久久精品一区二区三区| 嫩草影院入口| 日本五十路高清| 国产色爽女视频免费观看| 91在线精品国自产拍蜜月| 大型黄色视频在线免费观看| 亚洲天堂国产精品一区在线| 免费看美女性在线毛片视频| 两个人的视频大全免费| 久久久久久久久久久丰满| 99九九线精品视频在线观看视频| 久久精品91蜜桃| 欧美成人精品欧美一级黄| a级毛片免费高清观看在线播放| 中文亚洲av片在线观看爽| 国产v大片淫在线免费观看| 成年女人永久免费观看视频| 九九在线视频观看精品| 亚洲欧美精品综合久久99| 男女边吃奶边做爰视频| 精品不卡国产一区二区三区| 啦啦啦啦在线视频资源| 国产成人福利小说| 国产精品亚洲一级av第二区| 又爽又黄无遮挡网站| 国产一区二区在线av高清观看| 精品不卡国产一区二区三区| 国产精品久久久久久久久免| 九九热线精品视视频播放| 精品一区二区三区视频在线观看免费| 成熟少妇高潮喷水视频| 色综合站精品国产| 全区人妻精品视频| 一卡2卡三卡四卡精品乱码亚洲| 淫秽高清视频在线观看| 欧美日韩一区二区视频在线观看视频在线 | 国产麻豆成人av免费视频| 日韩欧美三级三区|