# Mechanistic Model and Optimization of the Diclofenac Degradation Kinetic for Ozonation Processes Intensification

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*Keywords:*modeling; kinetic study; ozonation; genetic algorithm; intensification

Modeling & Application of Advanced Oxidation Processes, Photocatalysis & Solar Photoreactors Engineering, Chemical Engineering Program, Universidad de Cartagena, Cartagena, 1382-Postal 195, Colombia

GAOX, CENM, Escuela de Ingeniería Química, Universidad del Valle, Cali 760032, Colombia

Research Group in Development of Materials and Products GIDENMP, CDT, ASTIN SENA, Tecnoparque 76003, Colombia

Author to whom correspondence should be addressed.

Academic Editor: Zacharias Frontistis

Received: 18 May 2021
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Revised: 9 June 2021
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Accepted: 11 June 2021
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Published: 15 June 2021

(This article belongs to the Special Issue Advances in Water and Wastewater Monitoring and Treatment Technology 2.0)

This work focused on estimating the rate constants for three ozone-based processes applied in the degradation of diclofenac. The ozonation (Oz) and its intensification with catalysis (COz) and photocatalysis (PCOz) were studied. Three mathematical models were evaluated with a genetic algorithm (GA) to find the optimal values for the kinetics constants. The Theil inequality coefficient (TIC) worked as a criterion to assess the models’ deviation. The diclofenac consumption followed a slow kinetic regime according to the Hatta number ($Ha<0.3$ ). However, it strongly contrasted with earlier studies. The obtained values for the volumetric rate of photon absorption (VRPA) corresponding to the PCOz process ($1.75\times {10}^{-6}$ & $6.54\times {10}^{-7}\mathrm{E}\mathrm{i}\mathrm{n}\mathrm{s}\mathrm{t}\mathrm{e}\mathrm{i}\mathrm{n}{\mathrm{L}}^{-1}\mathrm{m}\mathrm{i}{\mathrm{n}}^{-1}$ ) were significantly distant from the maximum ($2.59\times {10}^{-5}\mathrm{E}\mathrm{i}\mathrm{n}\mathrm{s}\mathrm{t}\mathrm{e}\mathrm{i}\mathrm{n}{\mathrm{L}}^{-1}\mathrm{m}\mathrm{i}{\mathrm{n}}^{-1}$ ). The computed profiles of chemical species proved that no significant amount of hydroxyl radicals was produced in the Oz, whereas the PCOz achieved the highest production rate. According to this, titanium dioxide significantly contributed to ozone decomposition, especially at low ozone doses. Although the models’ prediction described a good agreement with the experimental data ($\mathrm{T}\mathrm{I}\mathrm{C}<0.3$ ), the optimization algorithm was likely to have masked the rate constants as they had highly deviated from already reported values.

In the last two decades, an extensive list of pharmaceuticals and personal care products has ranked as contaminants of emerging concern (CECs). They have been frequently found in aqueous systems disrupting the normal development of the local biota [1,2,3]. The main concerns among these substances are their recalcitrant and cumulative behavior over the ecosystems. Nowadays, available technologies at industrial wastewater treatment plants (WWTPs) have not been enough to remove these pollutants from municipal effluents [4,5].

Advanced oxidation processes (AOPs) are well-known alternatives to deal with these types of compounds, which have been widely employed in the degradation of several CECs and proved to yield high degradation rates, even with removals over 99% at appropriate conditions [6,7,8,9]. Even so, AOPs still get challenged when it comes to the mineralization of recalcitrant compounds. This situation increases operational costs as more energy, reactive amount, and operation time are required [10,11,12].

However, the simultaneous application of AOPs can substantially improve degradation and mineralization by enhancing the production of highly oxidizing species. These processes are known as intensifications, and they have proved to considerably increase the production rate of hydroxyl radicals $\mathrm{H}{\mathrm{O}}^{\u2022}$ [13,14]. These processes have overcome kinetic limitations from traditional AOPs for a broad range of CECs from pharmaceutical, pesticidal, and petrochemical industries [15,16,17]. In addition, ozone-based intensifications are a promising field for wastewater treatments because it exploits the unstable behavior of the ozone molecules by promoting its interaction with UV and different types of catalysts such as zeolites, activated carbon, and semiconductors [18,19,20,21].

The catalytic and photocatalytic ozonation (COz and PCOz) are intensifications with a high synergetic effect. According to [22,23], their electrical consumption could be lower than the ozonation (Oz). Therefore, catalyst-based ozonation processes are attractive alternatives to improve water treatments. Although PCOz is a catalyst-based ozone process, the presence of photo-excitation leads to a more complex pathway. Thus, reactions at the catalyst surface occur by electron exchange with photo-excited active sites [24,25,26]. At the same time, COz reactions can also occur on non-excited active sites [27].

According to Yu et al., the amount of Lewis active sites (LAS) for a given catalyst significantly influences the degradation and mineralization during the COz [28,29,30]. Furthermore, for PCOz processes, a large amount of LAS could also increase the rate of capture of pairs electron-hole because of the high concentration of adsorbed ozone molecules, consequently increasing its oxidative potential [31]. Despite the current knowledge, these technologies are still being explored, and no industrial application has been proposed yet [32].

The kinetic studies on these processes have allowed a deeper insight into chemical and adsorption interactions. However, most of these studies have focused on setting operational ranges for critical variables, explaining synergy, and constructing feasible reaction mechanisms [22,25,33,34,35]. Meanwhile, few works have studied these processes from the field of mathematical modeling [26,36]. One of the main challenges for this approach is still the lack of information on kinetic rate constants. Therefore, in most cases, the use of traditional gradient-based methods to estimate these constants could be impractical because constraints are uncertain [37].

However, artificial intelligence (AI)-based methods such as genetic algorithms (GA) and particle swarm optimization (PSO) are feasible alternatives to overcome these problems. Nowadays, their popularity for solving multidimensional optimization problems has increased [38,39,40]. Several works have employed these methods for the estimation of kinetic rate constants. In 2019, Kadi et al. formulated a mathematical model to evaluate rapeseed oil transesterification. In their study, a PSO algorithm was employed [41]. Additionally, Ding et al. assessed both PSO and GA to model biomass pyrolysis based on 14 rate constants [42].

The present work proposed three mathematical models to degrade diclofenac using Oz, COz, and PCOz in a modified flotation cell. Twenty kinetic rate constants from [26,36] were estimated to complete the model. This study was a continuation of the work from Lara et al., where the experimental data to assess the models’ predictions were obtained [22]. The method employed to solve the optimization problem to find the rate constants was the Unified Non-dominated Sorting Genetic Algorithm (U-NSGA-III) proposed by [43].

The reaction mechanism for the ozonation process has been widely studied, even for different pH conditions. Staehelin et al. and Tomiyasu et al. proposed the first reaction mechanisms for ozone in water at acidic and alkaline conditions, respectively [44,45,46]. The significant difference between these pathways consisted of ozone decomposition reactions that occur because of alkalinity. However, because of the available variety of catalysts, the mechanisms for COz processes are less generalized. Jans and Hoigne carried the first known work in studying the effect of a catalyst over the ozonation process in 1998. Since then, different researchers have proposed feasible reaction paths based on the type of catalyst [47].

For the particular case of heterogeneous PCOz with titanium dioxide ($\mathrm{T}\mathrm{i}{\mathrm{O}}_{2}$), the available literature information is still scarce. Moreover, the already proposed mechanisms rely on independent knowledge over ozonation and heterogeneous photocatalysis mechanism [24,48]. Thus, this work collected part of this information to present a generalized mechanism, described in Table 1.

First, the homogeneous ozonation path was set to reactions (1)–(9), where both (1) and (2) had an initializing role. Then, the generated ozonide radicals ${\mathrm{O}}_{3}^{-\u2022}$ promoted the formation of hydroxyl radicals by reaction (3). It could consequently conduct homogeneous propagation reactions (5)–(9) or promote the hydroxyl attack on dissolved diclofenac molecules (4).

With the addition of $\mathrm{T}\mathrm{i}{\mathrm{O}}_{2}$, the process was also affected by heterogeneous reactions promoted by adsorption phenomena at the catalyst surface. Then, the COz mechanism was also described by reactions (14)–(18). As the hydroxide ions $\mathrm{O}{\mathrm{H}}^{-}$ were adsorbed on the catalyst, they were prone to react with ozone molecules to promote the production of hydroxyl radicals [49]. Furthermore, the heterogeneous hydroxyl attack reactions (16)–(18) additionally promoted the decomposition of diclofenac. However, as not enough information for adsorption kinetics was available, these reactions were modeled with a single global rate law.

Finally, UV radiation exposure led to the PCOz mechanism, which gathered photolysis and photocatalysis reactions. Here, the incidence of photons caused the catalyst excitation, where incident photons were likely to promote electrons at the catalyst valence band (VB) towards the conduction band (CB), which resulted in the formation of pairs electron-hole (19). The former allowed oxide-reduction reactions to take place. Thus, the holes promoted the generation of hydroxyl radicals by reactions (20) and (21), while electrons reacted with ozone to produce ozonide radicals (24). However, recombination of the photo-generated pair was also possible. Therefore, electrons could return to their VB (25). Meanwhile, at the homogeneous liquid phase, dissolved ozone was photolyzed (26), and the generated hydrogen peroxide was prone to react with hydroxyl radicals by (27).

The experimental measurements were obtained in a previous work from Lara et al. employing diclofenac sodium salt (${\mathrm{C}}_{14}{\mathrm{H}}_{10}\mathrm{C}{\mathrm{l}}_{2}\mathrm{N}\mathrm{N}\mathrm{a}{\mathrm{O}}_{2}$, >98%) as a preccursor for diclofenac [22]. The reaction system comprised an acrylic storage tank with a reaction volume ${\mathrm{V}}_{\mathrm{r}\mathrm{e}}=4.5$ $\mathrm{L}$, two fluorescent tubular lamps (Repti Glo 5.0 Compact) with a rated power of $20$ $\mathrm{W}$, and an Ozonator AZ2 model 5GLAB for ozone supply. This novel reactor has proven to involve turbulent zones which minimize the mass transfer limitations in the water treatments with ozone [50].

The flotation cell was modelled for the diclofenac degradation by Oz, COz, and PCOz. The predictions were compared against experimental data from [22], where the Oz process registered measures at ozone doses (${C}_{{O}_{3}}^{(in)}$) of 2.66 and 7.40 ppm. Meanwhile, the COz and PCOz processes employed a factorial design ${2}^{2}$ including the catalyst load (${C}_{mp}$) as a factor with levels 300 and 800 $\mathrm{ppm}$. The levels for the ozone dose factor were kept as equal as in the Oz.

According to Table 1, the mathematical models for each process were formulated based on: (i) absorption equilibrium, (ii) perfect mixing for both gas and liquid phases, (iii) little volatility for the water dissolved species, (iv) the catalyst particles were uniformly distributed, (v) the diclofenac photolysis was negligible, (vi) adiabatic conditions for the reaction system, (vii) the mass transfer resistance in the gas phase was negligible, (viii) continuous operation for the gas phase, (ix) batch operation for the liquid phase, (x) the ozone interface concentration described by Henry’s law ($\mathrm{He}$), and (xi) water and oxygen concentrations were considered constants as they were in excess.

Assumption (iii) implied that the models neglected the transport rate of the water-dissolved species to the gas phase. Then, ozone and oxygen were the only substances considered in the gas phase. The ozone accumulation rate was described according to (28), where the first and second terms, respectively, represented the net advective and the mixed convective-diffusive effects over the ozone transport to the liquid phase. The enhancement factor $E$ accounted for the increase in the ozone mass transfer rate because of the chemical reactions at the interface.

$$-{r}_{{O}_{3(g)}}=\frac{d{C}_{{O}_{3(g)}}}{dt}=\frac{{Q}_{(g)}}{{V}_{re}{\varphi}_{(g)}}({C}_{{O}_{3(g)}}^{(in)}-{C}_{{O}_{3(g)}})-{k}_{L}a({C}_{{O}_{3}}^{*}-{C}_{{O}_{3(l)}})E$$

The volumetric mass transfer coefficient ${k}_{L}a$ and the gas holdup ${\varphi}_{(g)}$ were computed with the empirical equations from Inkeri et al. for gassed stirred tank reactors [51], and the ozone gas flow-rate ${Q}_{(g)}$ was maintained fixed to $2.0$ $\mathrm{L}{\mathrm{min}}^{-1}$. Meanwhile, the ozone concentration at the interphase ${C}_{{O}_{3}}^{*}$ was a function of the mean logarithmic ozone gas concentration ${\overline{C}}_{{O}_{3(g)}}$, according to Equation (29).

$${C}_{{O}_{3}}^{*}={\overline{C}}_{{O}_{3(g)}}\frac{RT}{He}$$

Before evaluating the mathematical models, the Hatta number $(Ha)$ was computed for each of the experimental observations based on a first-order rate law according to Equation (30). Then, depending on the type of regime, the enhancement factor was computed [49]. Furthermore, the computed pseudo-first-order rate constant was employed to roughly estimate the electrical energy per order (EE/O) corresponding to each experimental configuration [52].

$$H{a}_{1}=\frac{\sqrt{k{D}_{{O}_{3}}}}{{k}_{L}}$$

Finally, the GA was applied, and the models’ predictions for the optimal rate constants were compared against the experimental data. Then, the Theil Inequality Coefficient ($\mathrm{TIC}$) was employed as a criterion to assess the models’ deviation as proposed by Beltrán et al., Equation (31). Values under 0.3 indicated a good agreement between the experimental measurements ${y}_{e}$ and the model’s predictions ${y}_{c}$ [36].

$$TIC=\frac{\sqrt{{\displaystyle {\sum}_{i}{({y}_{c,i}-{y}_{e,i})}^{2}}}}{\sqrt{{\displaystyle {\sum}_{i}{y}_{c,i}^{2}}}+\sqrt{{\displaystyle {\sum}_{i}{y}_{e,i}^{2}}}}$$

The degradation rate for the Oz process was mainly affected by the ozone and diclofenac concentrations $f({C}_{{O}_{3}},{C}_{DCF})$. Reactions (1)–(9) described the rate laws for the chemical species. Equation (32) described the resulting system of differential Equations $F$. Here, $R$ was a vector of rate laws, and $Z$ was a matrix of stoichiometric coefficients whose rows and columns represented the species and the kinetic rate constants each. Additionally, the element ${z}_{(n,m)}$ accounted for the ozone at the gas phase. All the remaining elements of the row $n$ and the column $m$ were zeros as none of the water-dissolved species could pass to the gas phase. The vector of initial conditions $Y$ was given to the model according to (35).

$$F=Z\times R$$

$$R=\left(\begin{array}{c}{r}_{1}={k}_{1}{\displaystyle \prod _{i=0}^{j}{C}_{i}}\\ {r}_{2}={k}_{2}{\displaystyle \prod _{i=0}^{j}{C}_{i}}\\ \vdots \\ {r}_{m-1}={k}_{m-1}{\displaystyle \prod _{i=0}^{j}{C}_{i}}\\ {r}_{{O}_{3(g)}}\end{array}\right)$$

$$Z=\left(\begin{array}{ccccc}{z}_{1,1}& {z}_{1,2}& \cdots & {z}_{1,n-1}& 0\\ {z}_{2,1}& {z}_{2,2}& \cdots & {z}_{2,n-1}& 0\\ \vdots & \vdots & \ddots & \vdots & \vdots \\ {z}_{m-1,1}& {z}_{m-1,2}& \cdots & {z}_{m-1,n-1}& 0\\ 0& 0& \cdots & 0& -1\end{array}\right)$$

$$Y={\left(\begin{array}{cccccccccc}{C}_{DCF},& {C}_{{O}_{3}(l)},& {C}_{{H}^{+}},& {C}_{O{H}^{-}},& {C}_{{O}_{3}^{-\u2022}},& {C}_{H{O}^{\u2022}},& {C}_{H{O}_{2}^{-}},& {C}_{H{O}_{2}^{\u2022}},& {C}_{{O}_{2}^{-\u2022}},& {C}_{{O}_{3}(g)}\end{array}\right)}^{T}$$

The catalytic ozonation model was also a function of the catalyst load $f({C}_{{O}_{3}},{C}_{DCF},{C}_{mp})$. Reactions (1)–(9) and (14)–(18) described the set rate laws. According to the general assumptions from Section 3, the adsorption-desorption rates at the catalyst surface were at equilibrium with the liquid phase. Therefore, the concentration of adsorbed species was described in terms of the homogeneous concentration (36).

$${C}_{S-DCF}={K}_{ap{p}_{1}}{C}_{DCF}$$

As the heterogeneous reactions were surface interactions, its rate laws relied on the available surface rather than the reaction volume. Therefore, a dimensionality factor was required to represent the global volumetric effect of these interactions based on the load and specific surface of the catalyst ${C}_{mp}{S}_{g}$. Then, the $R$ vector was modified according to (37). The corresponding $Z$ matrix was constructed similarly to (34), but rather than $m$ chemical reactions, it was composed by $m+h$, where $h$ was the total number of heterogeneous chemical reactions. The $Y$ vector for the initial condition was the same as that from (35).

$$R=\left(\begin{array}{c}{r}_{1}={k}_{1}{\displaystyle \prod _{i=1}^{j}{C}_{i}}\\ \vdots \\ {r}_{m-1}={k}_{m}{\displaystyle \prod _{i=1}^{j}{C}_{i}}\\ {r}_{{h}_{1}}={C}_{mp}{S}_{g}{k}_{m+1}^{(het)}{\displaystyle \prod _{i=1}^{j}{C}_{i}}\\ \vdots \\ {r}_{{h}_{l}}={C}_{mp}{S}_{g}{k}_{m+l}^{(het)}{\displaystyle \prod _{i=1}^{j}{C}_{i}}\\ {r}_{{O}_{3(g)}}\end{array}\right)$$

The PCOz process was additionally affected by the rate of photon absorption, which was quantified using the volumetric rate of photon absorption (VRPA). Therefore, the model was a function $f({C}_{{O}_{3}},{C}_{DCF},{C}_{mp},VRPA)$ based on reactions (1)–(9), (14)–(21), (22) and (24)–(27). Equations (38) and (39) depict the formulation for the $R$ vector and the $Y$ matrix.

$$R=\left(\begin{array}{c}{r}_{1}={k}_{1}{\displaystyle \prod _{i=1}^{j}{C}_{i}}\\ \vdots \\ {r}_{{h}_{1}}={C}_{mp}{S}_{g}{k}_{m+1}^{(het)}{\displaystyle \prod _{i=1}^{j}{C}_{i}}\\ \vdots \\ {r}_{UV}={\varphi}_{{O}_{3}}{C}_{{O}_{3}}\\ {r}_{Ti}=VRPA\\ {r}_{{O}_{3(g)}}\end{array}\right)$$

$$Y={\left(\begin{array}{ccccccccccccc}{C}_{DCF},& {C}_{{O}_{3}(l)},& {C}_{{H}^{+}},& {C}_{O{H}^{-}},& {C}_{{O}_{3}^{-\u2022}},& {C}_{H{O}^{\u2022}},& {C}_{H{O}_{2}^{-}},& {C}_{H{O}_{2}^{\u2022}},& {C}_{{O}_{2}^{-\u2022}},& {C}_{{h}^{+}},& {C}_{{e}^{-}},& {C}_{{H}_{2}{O}_{2}},& {C}_{{O}_{3}(g)}\end{array}\right)}^{T}$$

Although reaction (23) has an active role in heterogeneous photocatalysis processes, it was assumed negligible compared to (24). Hence, it was supposed that most of the active sites $Ti(III)$ would take preference to interact with ozone rather than oxygen molecules [36]. The reaction (22) was considered at equilibrium. Therefore, the concentration of active sites was quantified in terms of the electron concentration ${C}_{{e}^{-}}$, Equation (40).

$${C}_{Ti(III)}={K}_{ap{p}_{x}}{C}_{{e}^{-}}$$

A fundamental part of modeling photocatalysis-based processes is the quantification of the VRPA. Among the literature, researchers have widely aborded stochastic and deterministic approaches estimating the VRPA [53,54,55]. Although stochastic methods based on Monte Carlo simulations have proved highly precise, their implementation involves a high computational effort, resulting in a time-consuming task [56,57,58,59]. Meanwhile, some deterministic methods have proved to yield prediction approximated enough to Monte Carlo simulations. Among these methods, the Six-Flux Model (SFM) has been successfully adapted to different photoreactor geometries [60,61,62,63,64].

As the study of the radiant field was not the main objective of this work, the estimation of the VRPA at the flotation cell followed the SFM approach (See Section S.1). The optical properties of the catalyst were obtained from [61]. Equation (41) describes the local volumetric rate of photon absorption (LVRPA) for each lamp as a function of the intensity ${I}_{0}$.

$$LVRP{A}_{i}=\frac{{I}_{0}}{{\lambda}_{corr}{\omega}_{corr}(1-\gamma )}\left[\left({\omega}_{corr}-1+\sqrt{1-{\omega}_{corr}}\right){e}^{-({r}_{p}(r,\theta )/{\lambda}_{corr})}+\gamma \left({\omega}_{corr}-1-\sqrt{1-{\omega}_{corr}}\right){e}^{({r}_{p}(r,\theta )/{\lambda}_{corr})}\right]$$

As the studied system comprised two non-concentric lamps, Equation (42) re-defined the relative coordinate to the emission source ${r}_{p}$ as a composed coordinate ${r}_{p}(r,\theta )$, where the constant $a$ was the distance from the reactor center to the emission source.

$${r}_{p}(r,\theta )=\sqrt{{r}^{2}+{(a/2)}^{2}-ar\cdot \mathrm{cos}(\theta )}$$

Then, to account for the effect of both emission sources, the real LVRPA value for a given point inside the flotation cell was computed as the summation of the individual lamp’s contribution, Equation (43). The overall rate of photon absorption in the system (VRPA) was given by Equation (44) [63]. Figure 1 depicts the geometry for the studied system.

$$LVRP{A}_{T}=LVRP{A}_{1}+LVRP{A}_{2}$$

$$VRPA=\frac{{\displaystyle {\int}_{0}^{r}{\displaystyle \underset{0}{\overset{2\pi}{\int}}LVRP{A}_{T}d\theta dr}}}{{\displaystyle {\int}_{0}^{r}{\displaystyle \underset{0}{\overset{2\pi}{\int}}d\theta dr}}}$$

The kinetic parameters were estimated by the U-NSGA-III algorithm from the Pymoo library of Python [65]. Seada and Deb initially proposed this method in 2016 to deal with mono and multi-objective optimization problems [43]. The objective function was the weighted least squares shown in Equation (45). The index $M$ accounted for the involved processes (Oz, COz, and PCOz), ${r}_{i,j}$ were the residual values, and ${\sigma}_{i,j}$ was the experimental variance for the ${i}^{th}$ experiment at the ${j}^{th}$ measurement.

$${\Sigma}_{T}={\displaystyle \sum _{M}{\displaystyle \sum _{i=1}^{2}{\displaystyle \sum _{j=1}^{n}\frac{{\left({r}_{i,j}^{(M)}\right)}^{2}}{{\sigma}_{i,j}^{2}}}}}$$

Algorithm 1 described pseudocode for the case of the present optimization problem. Both population size and the maximum number of iterations were set to 150. First, the algorithm distributed an initial population $P$ of vector parameters ${p}_{i}$ within the problem space and evaluated its associated error. Then, the offspring were generated based on binary tournament selection events. Each winner from a tournament was matched with an individual from another tournament, resulting in two offspring individuals ${c}_{1}$ and ${c}_{2}$ [43].

Algorithm 1 Pseudocode for the application of the U-NSGA-III. |

Degenerated U-NSGA-III |

Inputs: Mono-objective problem ${\sum}_{T}$, experimental data $\widehat{Y}$, Boundaries for the problem space $\left({X}_{\mathrm{min}},{X}_{\mathrm{max}}\right)$, and known physicochemical constants. Output: Best explored solution ${p}_{best}$ |

$P=Initialize(N=150)$ |

$Evaluate(P)$ |

while $generation\le 150$ do |

$Q=\varnothing $ |

while $\left|Q\right|<\left|P\right|$ do |

${p}_{1}=TournamentSelect(P)$ |

${p}_{2}=TournamentSelect(P)$ |

$\left({c}_{1},{c}_{2}\right)=recombination({p}_{1},{p}_{2})$ |

${c}_{1}=mutate({c}_{1})$ |

${c}_{2}=mutate({c}_{2})$ |

$Q\cup \left\{{c}_{1},{c}_{2}\right\}$ |

end while |

$Evaluate(Q)$ |

$P=best(P\cup Q)$ |

end while |

${p}_{best}=best(P)$ |

Before introducing the obtained pair of candidates to the offspring set $Q$, the algorithm applied mutation operators over the vectors. This approach helps the algorithm keep diversity between individuals and improves the exploration of the problem space [66]. Once $Q$ equaled the size of $P$, the algorithm computed the error for the offspring individuals. Finally, a new population was constituted by selecting the best candidates from $Q$ and $P$. This methodology continued until the maximum number of generations was met.

A sensitivity analysis was employed to study the effect of each kinetic constant on the models’ error. The corresponding sensitivity coefficients were used as criteria to neglect poor influential chemical reactions. Although global sensitivity analysis algorithms are preferred since they provide more valuable information [67], the local-based methods had the advantage of quick computing and easy applicability. Therefore, a one-at-a-time (OAT) approach was implemented to estimate the sensitivity coefficients for the rate constants. Hence, the number of samples was set to $M=500$, and the error was evaluated while varying one rate constant and keeping the remaining fixed to their optimal values. Then, the variance of the error for that constant was computed [68,69]. Thus, the corresponding sensitivity coefficients $S({k}_{i})$ were estimated based on Equation (46).

$$S({k}_{i})\approx \frac{Var({\sum}_{T}|{k}_{i})}{Var({\sum}_{T})}=\frac{Var({\sum}_{T}|{k}_{i})}{{\displaystyle \sum _{i}^{n}Var({\sum}_{T}|{k}_{i})}}$$

All the processes described a slow kinetic regime ($Ha<0.3$). Therefore, no significant enhancement of the mass transfer occurred by the chemical reactions at the gas-liquid interface ($E\approx 1$). The values for the mass transfer parameters and the computed values for the Ha corresponding to each experiment were reported in Sections S.2 and S.3 of the Supplementary Material, respectively.

The EE/O in terms of diclofenac degradation for the COz and PCOz were lower than the Oz process only when operating at high ozone dose conditions. COz presented the lowest EE/O, with a value of 7.22 $\mathrm{k}\mathrm{W}\mathrm{h}$ ${\mathrm{m}}^{-3}$ for 7.44 ppm ozone dose and 800 ppm catalyst load, which suggested that these conditions promoted the fastest degradation (See Section S.4).

The ozonation model was constructed based on the reactions (1)–(9), resulting in the system of ordinary differential equations (ODEs) from Equation (47). Table 2 reported the values for the involved reaction rate constants.

$${F}_{Oz}=\left(\begin{array}{l}\frac{d{C}_{DCF}}{dt}=-\left({k}_{1}{C}_{{O}_{3(l)}}+{k}_{4}{C}_{H{O}^{\u2022}}\right){C}_{DCF}\\ \frac{d{C}_{{O}_{3(l)}}}{dt}={k}_{L}a({C}_{{O}_{3}}^{*}-{C}_{{O}_{3(l)}})-\left({k}_{1}{C}_{DCF}+{k}_{2}{C}_{O{H}^{-}}+{k}_{5}{C}_{H{O}^{\u2022}}+{k}_{7}{C}_{H{O}_{2}^{-}}+{k}_{7}{C}_{{O}_{2}^{-\u2022}}\right){C}_{{O}_{3(l)}}\\ \frac{d{C}_{{H}^{+}}}{dt}={k}_{8}{C}_{H{O}_{2}^{\u2022}}-\left({k}_{3}{C}_{{O}_{3}^{-\u2022}}+{k}_{-8}{C}_{{O}_{2}^{-\u2022}}\right){C}_{{H}^{+}}\\ \frac{d{C}_{O{H}^{-}}}{dt}={k}_{6}{C}_{H{O}_{2}^{-}}{C}_{H{O}^{\u2022}}-{k}_{2}\frac{{K}_{w}}{{C}_{{H}^{+}}}{C}_{{O}_{3(l)}}\\ \frac{d{C}_{{O}_{3}^{-\u2022}}}{dt}=\left({k}_{1}{C}_{DCF}+{k}_{7}{C}_{H{O}_{2}^{-}}+{k}_{9}{C}_{{O}_{2}^{-\u2022}}\right){C}_{{O}_{3(l)}}-{k}_{3}{C}_{{O}_{3}^{-\u2022}}{C}_{{H}^{+}}\\ \frac{d{C}_{H{O}^{\u2022}}}{dt}={k}_{3}{C}_{{O}_{3}^{-\u2022}}{C}_{{H}^{+}}-\left({k}_{4}{C}_{DCF}+{k}_{5}{C}_{{O}_{3(l)}}+{k}_{6}{C}_{H{O}_{2}^{-}}\right){C}_{H{O}^{\u2022}}\\ \frac{d{C}_{H{O}_{2}^{-}}}{dt}={k}_{2}{C}_{O{H}^{-}}{C}_{{O}_{3(l)}}-\left({k}_{6}{C}_{H{O}^{\u2022}}+{k}_{7}{C}_{{O}_{3(l)}}\right){C}_{H{O}_{2}^{-}}\\ \frac{d{C}_{H{O}_{2}^{\u2022}}}{dt}=\left({k}_{4}{C}_{DCF}+{k}_{5}{C}_{{O}_{3(l)}}\right){C}_{H{O}^{\u2022}}+\left({k}_{6}{C}_{H{O}^{\u2022}}+{k}_{7}{C}_{{O}_{3(l)}}\right){C}_{H{O}_{2}^{-}}+{k}_{-8}{C}_{{O}_{2}^{-\u2022}}{C}_{{H}^{+}}-{k}_{8}{C}_{H{O}_{2}^{\u2022}}\\ \frac{d{C}_{{O}_{2}^{-\u2022}}}{dt}={k}_{8}{C}_{H{O}_{2}^{\u2022}}-\left({k}_{-8}{C}_{{H}^{+}}+{k}_{9}{C}_{{O}_{3(l)}}\right){C}_{{O}_{2}^{-\u2022}}\\ \frac{d{C}_{{O}_{3(g)}}}{dt}=\frac{{Q}_{(g)}}{{V}_{re}{\varphi}_{(g)}}({C}_{{O}_{3(g)}}^{(in)}-{C}_{{O}_{3(g)}})-{k}_{L}a({C}_{{O}_{3(g)}}-{C}_{{O}_{3}}^{*})\end{array}\right)$$

Although the estimated values in the present work had a good agreement with the experimental data, their values highly deviated from already reported kinetic constants for the Oz process.

The sensitivity analysis showed that only reaction (1) had a significant effect on the Oz model. Its sensitivity coefficient presented a value over 0.9, as depicted in Figure 2. Thus, the mechanism was reduced to a single homogeneous reaction given by (1). The resulting mathematical model was only dependent on the ozone and diclofenac concentrations.

Both complex and simplified models fitted the diclofenac degradation kinetic. Nevertheless, for the high ozone dose conditions (7.40 ppm), the model deviation increased because of the high sensitivity to the ozone concentration. Figure 3 depicted the concentration profiles. According to Figure 3b, no ozone decomposition occurred. It explained the negligible influence of the hydroxyl radicals on the diclofenac degradation.

In addition to (1)–(9), the rate laws from (14)–(18) affected the COz process. Then, the corresponding system of differential equation was formulated as a function of ${F}_{Oz}$, Equation (48). The optimal values for the heterogeneous rate constants were presented in Table 3. Due to the lack of information, their values could not be compared with literature.

$${F}_{COz}={F}_{Oz}+\left(\begin{array}{l}-{C}_{mp}{S}_{g}{k}_{12}{C}_{DCF}{C}_{H{O}^{\u2022}}\\ -{C}_{mp}{S}_{g}{k}_{10}{C}_{O{H}^{-}}{C}_{{O}_{3}}\\ -{C}_{mp}{S}_{g}{k}_{11}{C}_{{O}_{3}^{-\u2022}}{C}_{{H}^{+}}\\ -{C}_{mp}{S}_{g}{k}_{10}{C}_{O{H}^{-}}{C}_{{O}_{3}(l)}\\ {C}_{mp}{S}_{g}\left({k}_{10}{C}_{O{H}^{-}}{C}_{{O}_{3}(l)}-{k}_{11}{C}_{{O}_{3}^{-\u2022}}{C}_{{H}^{+}}\right)\\ {C}_{mp}{S}_{g}\left({k}_{10}{C}_{O{H}^{-}}{C}_{{O}_{3}(l)}+{k}_{11}{C}_{{O}_{3}^{-\u2022}}{C}_{{H}^{+}}-{k}_{12}{C}_{DCF}{C}_{H{O}^{\u2022}}\right)\\ 0\\ 0\\ 0\\ 0\end{array}\right)$$

According to the sensitivity coefficients from Figure 4, the reaction mechanism for the catalytic ozonation process was simplified by just considering (1), (5), (8) and (9)–(11) to affect the mathematical model.

The low concentration at the ozone dose (2.66 ppm) caused the decomposition at the catalyst surface (14) to compete with the direct diclofenac destruction by ozone (1), Figure 5a. It occurred for both experimental and predicted data. However, for high ozone dose conditions (7.44 ppm), the ozone availability could drive the diclofenac degradation without competing. Additionally, Figure 5b showed that the ozone decomposition at these conditions was negligible.

As the change in the number of active sites affects the adsorption equilibrium of catalytic reactions, the increase in the catalyst load led to a lower accumulation of dissolved ozone. Furthermore, the high ozone dose conditions did not promote the formation of hydroxyl radicals. Based on this, the ozone excess conditions could have led reaction (5) to become a scavenging pathway for the hydroxyl radicals. The former suggested that the ozone concentration had a strong influence on the kinetic behavior of the process.

The catalyst particles near the emission sources strongly screened the photons for outer particles. Thus, the LVRPA for the catalyst particle near the walls of the flotation cell was almost null. Figure 6 depicted the computed distribution of the LVRPA for a transversal view of the reactor at catalyst loads of 10, 50, 100, and 800 ppm.

According to these observations, the range of catalyst loads employed was far from the VRPA optimal value. Figure 7 confirmed it, as it showed that the maximum value for the VRPA was located at 12 ppm.

The mathematical model was fed with the dataset from Figure 7 to interpolate the corresponding VRPA value given the catalyst load. The resulting system was constructed in terms of ${F}_{COz}$. The photolysis and photocatalysis reactions from Table 1 were included according to (49).

$${F}_{PCOz}=\left(\begin{array}{c}{f}_{CO{z}_{1}}\\ {f}_{CO{z}_{2}}\\ {f}_{CO{z}_{3}}\\ {f}_{CO{z}_{4}}\\ {f}_{CO{z}_{5}}\\ {f}_{CO{z}_{6}}\\ {f}_{CO{z}_{7}}\\ {f}_{CO{z}_{8}}\\ {f}_{CO{z}_{9}}\\ 0\\ 0\\ 0\\ {f}_{CO{z}_{10}}\end{array}\right)+\left(\begin{array}{l}-{C}_{mp}{S}_{g}{k}_{12}{C}_{DCF}{C}_{H{O}^{\u2022}}\hfill \\ -{C}_{mp}{S}_{g}{k}_{15}{C}_{{e}^{-}}{C}_{{O}_{3}(l)}-{\varphi}_{{O}_{3}}\hfill \\ {C}_{mp}{S}_{g}{k}_{14}{C}_{{e}^{-}}\hfill \\ 0\hfill \\ {C}_{mp}{S}_{g}{k}_{15}{C}_{{e}^{-}}{C}_{{O}_{3}(l)}\hfill \\ {C}_{mp}{S}_{g}\left({k}_{14}{C}_{O{H}^{-}}{C}_{{e}^{-}}-{k}_{12}{C}_{DCF}{C}_{H{O}^{\u2022}}\right)-{k}_{17}{C}_{{H}_{2}{O}_{2}}{C}_{H{O}^{\u2022}}\hfill \\ 0\hfill \\ {k}_{17}{C}_{{H}_{2}{O}_{2}}{C}_{H{O}^{\u2022}}\hfill \\ 0\hfill \\ VRPA-{C}_{mp}{S}_{g}\left({k}_{13}{C}_{O{H}^{-}}+{k}_{14}+{k}_{15}{C}_{{O}_{3}(l)}+{k}_{16}{C}_{{e}^{-}}\right){C}_{{h}^{+}}\hfill \\ VRPA-{C}_{mp}{S}_{g}{k}_{15}{C}_{{O}_{3}(l)}{C}_{{e}^{-}}\hfill \\ {\varphi}_{{O}_{3}}{C}_{{O}_{3}(l)}-{k}_{17}{C}_{{H}_{2}{O}_{2}}{C}_{H{O}^{\u2022}}\hfill \\ 0\hfill \end{array}\right)$$

The optimal values for the photocatalysis and photolysis rate constants were summarized in Table 4. According to Figure 8, the simplified mechanism only included reactions (1), (8), (9), (14), (15), (21), (26) and (27). The participation of (25) acted as a route for radical hydroxyl consumption with a higher probability than (16).

Again, the ozone excess allowed the direct diclofenac destruction by ozone to dominate the process kinetics. However, the degradation kinetic was even slower for the low ozone dose than observed in the COz process. It was attributed to the ozone photolysis reaction. Figure 9 presents the concentration profiles for each of the experiment configurations. Because of the photolysis, ozone accumulation was slower compared with the COz and Oz processes. Besides, from Figure 9d, the production of hydrogen peroxide was observed, which suggested the active role of the photolysis reaction.

According to the EE/O estimates in terms of degradation, the PCOz and COz processes could save electrical consumption compared to the Oz process only when there was enough ozone in the system to carry direct diclofenac destruction by ozone, reaction (1), without competing with the decomposition reactions (7.40 ppm). Although COz presented the lowest EE/O, the authors encourage further estimations of the EE/O in terms of TOC removal in order to fairly compare these processes, according to the work from Yu et al. [31].

The kinetic rate constants from Table 2 described a high discrepancy with the values reported in the literature. It suggested that the proposed mathematical model overestimated the rate at which the ozone molecules reacted in the system. Thus, the optimization algorithm weighted this situation by giving lower values to the kinetic constants and fit the experimental data.

According to Beltran et al., the ozonation of diclofenac describes a fast kinetic regime. Although this contrasted the current results, a fast kinetic regime would explain the expected high value of the homogeneous kinetic constants. The former would imply that a significant amount of ozone must react at the gas-liquid interface before dissolving [36]. Then, a different mathematical approach would be required to deal with the microscopic material balance, i.e., Benbelkacem et al. proposed to simultaneously integrate the microscopic and reactor material balances and compute the enhancement and depletion factors for each time step [70].

To the best of the authors’ knowledge, no experimental data was reported to compare the heterogeneous and photolysis rate constants. However, it was observed that the catalyst played a significant role in the production of hydroxyl radicals by ozone decomposition. The main reason was the use of a metallic-oxide-based catalyst as it is known to promote electron transfer because of the formation of functional groups at the surface of the catalyst [71].

On the other hand, the photocatalysis rate constants had negligible values compared to ${k}_{10}^{(het)}$ and ${k}_{11}^{(het)}$. It suggested that photocatalysis yielded a poor influence on the diclofenac degradation. This idea was in agreement with [22]. In their observations, the photocatalysis of diclofenac yielded the slowest degradation. The $\mathrm{T}\mathrm{i}{\mathrm{O}}_{2}$ bandgap could explain this behavior as it limits the catalyst photoactivity [72,73,74].

Meanwhile, (27) was a potential path for scavenging hydroxyl radicals according to the value of ${k}_{17}$. It was the highest value within the estimated rate constants, with a magnitude even higher than the reported value [36], exhibiting an error superior to 100%. Nevertheless, earlier studies have met this kind of discrepancy, i.e., Huber et al. reported that ${k}_{1}\approx 6\times {10}^{8}{\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$. Meanwhile, Sein et al. and Zhaoxu et al. have reported values of $4.1\times {10}^{7}{\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$ and $1.54\times {10}^{5}{\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$, respectively [35,75,76]. Even so, it was not discarded that the optimization algorithm could mask ${k}_{17}$ to fit the experimental data. Therefore, more information about the processes is required to establish more robust constraints over the optimization problem.

No asseveration regarding the degradation products could be established as they were not experimentally measured. However, it was expected the occurrence of hydroxylated diclofenac species, mainly 5-hydroxydiclofenac, which is more reactive than its isomer 4-hydroxidiclonac that is produced during the metabolization of diclofenac [77,78]. The major concern about this degradation product of diclofenac is that it could be further oxidated into quinone imine derivatives, which are suspected to be responsible for the diclofenac toxic effects [7,79].

The ozone dose condition limited the model accuracy. Nevertheless, the model predicted the experimental data within an acceptable error margin. For the case of the experimental conditions, the Theil inequality coefficient was under 0.3. Thus, there was a good agreement with the studied data. According to Figure 3a, the mathematical model overestimated the ozone effect over the diclofenac degradation. The fact that the mechanism did not consider intermediate species may have influenced the model predictions. Earlier studies on the diclofenac degradation with ozone have demonstrated that intermediates such as aminyl radicals and hydroxylated diclofenac derivatives affect the process kinetics [35,77].

The negligible influence over the diclofenac degradation presented by ${k}_{3}$ and ${k}_{4}$ (Figure 2) explained the absence of ozone decomposition in Figure 3b. However, this contrasted with Flyunt et al., as it is expected that ozone processes will yield hydroxyl radicals [80]. Additionally, the hydroxyl radicals are likely to attack the aromatic ring because of their electrophilic nature. According to Sein et al., the hydroxyl radicals can initiate a mechanism for the production of 5-hydroxydiclofenac [35]. Therefore, the optimization problem required more accurate constraints based on the concentration of additional chemical species.

According to Figure 5a,b, the catalyst supported the ozone decomposition, but this process was susceptible to the ozone dose. Thus, no decomposition occurred at 7.40 ppm ${O}_{3(g)}^{(in)}$. Following the sensitivity analysis of Figure 4, the direct diclofenac destruction by ozone (1) was not the most influential over the mechanism for this model. Instead, reaction (15) assumed this role. Then, for the case of 2.66 ppm ${O}_{3(g)}^{(in)}$ ozone was not in excess and diclofenac molecules had to compete with (14), whose rate constant was three orders of magnitude above ${k}_{1}$. Thus, for these conditions, the diclofenac degradation was slower. In addition, the increase in the catalyst load made the degradation rate even slower as a large surface was available for reaction (14).

Although the ozone excess in the system enhanced the diclofenac degradation rate, Figure 5c showed that such conditions did not promote a significant generation of hydroxyl radicals; however, the high value of ${k}_{11}^{(het)}$ suggested the opposite. According to this, it was likely that a deficit of hydrogen ions limited the rate of reaction (15). Figure 5d supported this hypothesis as it did not show consumption of the ozonide radicals ${O}_{3}^{-\u2022}$. Then, the rate of reactions (3) and (9) was negligible. The former contrasted most of the research in COz processes [34]. Nevertheless, it should not be discarded that unfavorable setting of the operational conditions can lead processes to poor performance. According to this, not all the ozone doses favored mineralization.

Based on the model’s simplifications, it was stated that the OAT sensitivity analysis did not provide enough information to discard kinetic constants without affecting the model outputs. Thus, the sensitivity analysis required a more robust analysis based on global methods to assess the interaction between parameters [67,81]. The most significant discrepancy of the simplified model was observed in Figure 5d, where the trend of concentration profiles described a completely different behavior. However, predictions for the diclofenac remained unchanged as the hydroxyl attack reactions (4) and (16) did not influence this output.

As observed in Figure 6, the catalyst particles were likely to screen the photon flux for particles near the reactor walls. Consequently, further research should weigh the available number of active sites against the VRPA to find optimal operation conditions. According to Figure 7, the catalyst loads employed in this work were considerably distant from the computed optimum value for the VRPA. However, considering the results for the COz model, a reduction in the catalyst load could also reduce the number of active sites. It was observed that the behavior described in Figure 7 was analogous to the results from Colina et al. [61], which supported the proposed methodology to estimate the VRPA in cases of multiple non-concentric lamps with annular photoreactors.

The only considerable photocatalytic reaction was (21). Meanwhile, the reactions induced by photolysis both seemed to affect the model outputs. Due to the number of interactions, the diclofenac degradation was slower than the COz. Figure 9b showed that reactions (14) and (27) produced a fast decay in the ozone accumulation. This effect was scaled with the catalyst load employed, as a larger surface was available for reaction (14) to occur.

Additionally, from Figure 9c, it was observed for the cases of high ozone dose that the concentration of hydroxyl radicals increased suddenly when the dissolved ozone concentration approximated to zero. The attained accumulation was higher than that observed in the COz model. Meanwhile, the accumulation predicted for the hydrogen peroxide described a similar behavior to the observations from Peyton and Glaze for ozone photolysis on distilled water [82]. However, for the present work, the equilibrium concentration dropped to zero, Figure 9d. Finally, as observed in the COz model, the simplification based on the sensitivity analysis added no significant error in the diclofenac concentration, but outputs for other chemical species changed considerably.

Through this study, a generalized reaction pathway for ozone and ozone-catalyst-based processes was proposed. The mechanism could describe the degradation kinetics for all the experiments in the modified flotation cell for different configurations of the ozone dose and the catalyst load. The models might be extended for applications with other metal oxide-based catalysts. However, it is worth noting that optical and surface properties should be replaced and the kinetic constants accounting for surface reactions should be estimated.

Although the employed experimental equations for the calculation were proposed for stirred tanks, they proved to describe ozone unreactive transport from the gas to the liquid phase for the current experimental conditions. However, the computed slow kinetic regime was discordant to the established theories from previous works. Therefore, it was stated that a first-order rate law was not a determinant criterion to characterize kinetic regimes for ozone-based processes applied in the degradation of diclofenac.

The proposed approach for the VRPA estimation stood valid within the employed range of experimental variables of the current study and for the proposed mathematical models, although no formal validation was designed. Nevertheless, the selected values of the catalyst load were far from yielding an optimum for the VRPA.

No premature convergence was observed in estimating the rate constants; this suggested a high probability of reaching a global minimum for the objective function (18). In addition, all the experiments presented a $\mathrm{TIC}<0.3$. The former was traduced as a strong agreement between predictions and experimental data. Nevertheless, the homogeneous rate constants were discordant with the already reported values, which suggested that the optimization algorithm masked the magnitudes of the constants to fit the data.

Only the Oz process accepted the simplifications based on the sensitivity analysis without considerable changes on their outputs. However, for predictive purposes of the diclofenac concentration, the three simplified models could be employed within the current experimental conditions.

The PCOz promoted a higher amount of hydroxyl radical than the COz. However, this production only became significant when all the dissolved ozone was consumed. Moreover, more research is required to establish the optimal experimental configuration for the PCOz to exploit photoactivity and surface availability. The use of UVB/UVC could improve the rate of photocatalysis reactions.

The following are available online at https://www.mdpi.com/article/10.3390/w13121670/s1, Figure S1: First-order rate law predictions for the diclofenac concentration in the ozonation process, Figure S2: First-order rate law predictions for the diclofenac concentration in the catalytic ozonation process, Figure S3: First-order rate law predictions for the diclofenac concentration in the photocatalytic ozonation process, Table S1: Constants employed to estimate the LVRPA, Table S2: Mass transfer constants for the flotation cell, Table S3: Electrical energy per order (EE/O) for each process conditions.

Conceptualization, J.L.-R., M.A.M., and F.M.-M.; methodology, B.A.-A., J.L.-R., and J.D.-A. validation, B.A.-A. and J.L.-R.; formal analysis, B.A.-A., J.L.-R., and J.D.-A.; investigation, B.A.-A. and J.L.-R.; writing—original draft preparation, B.A.-A.; writing—review and editing, B.A.-A., J.L.-R., and F.M.-M.; supervision, M.A.M. and F.M.-M.; project administration, F.M.-M.; funding acquisition, F.M.-M. All authors have read and agreed to the published version of the manuscript.

This paper was supported by Universidad del Valle (Colombia) and Sistema General de Regalias SGR (Colombia) with the projects CI. 2987 and Grant BPIN 2018000100096.

Not applicable.

Not applicable.

Restrictions apply to the availability of these data. Data was obtained from [third party] and are available [from the authors/at URL] with the permission of [third party].

The author thanks Tecnoparque Nodo Cali and Universidad del Valle. Diaz-Angulo and Lara Ramos thank the Ministerio de Ciencia Tecnología e Innovación for the Ph.D. Scholarship 647, 727 and for the financial support to produce this work through the project CI. 2987 and BPIN 2018000100096.

The authors declare no conflict of interest.

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Reaction Mechanism | |||
---|---|---|---|

Homogeneous Initialization | Heterogeneous attack of $\mathrm{H}{\mathrm{O}}^{\u2022}$ | ||

${\mathrm{O}}_{3}+\mathrm{D}\mathrm{C}\mathrm{F}\stackrel{{\mathrm{k}}_{1}}{\to}\mathrm{P}+{\mathrm{O}}_{3}{}^{-\u2022}$ | (1) | $\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-\mathrm{H}{\mathrm{O}}^{\u2022}+\mathrm{D}\mathrm{C}\mathrm{F}-\mathrm{S}\stackrel{{\mathrm{k}}_{12}{}^{(\mathrm{h}\mathrm{e}\mathrm{t})(\mathrm{a})}}{\to}\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})+\mathrm{P}-\mathrm{S}$ | (16) |

${\mathrm{O}}_{3}+\mathrm{O}{\mathrm{H}}^{-}\stackrel{{\mathrm{k}}_{2}}{\to}\mathrm{H}{\mathrm{O}}_{2}{}^{-}+{\mathrm{O}}_{2}$ | (2) | $\mathrm{H}{\mathrm{O}}^{\u2022}+\mathrm{D}\mathrm{C}\mathrm{F}-\mathrm{S}\stackrel{{\mathrm{k}}_{12}{}^{(\mathrm{h}\mathrm{e}\mathrm{t})(\mathrm{b})}}{\to}\mathrm{P}-\mathrm{S}$ | (17) |

Homogeneous production of $\mathrm{H}{\mathrm{O}}^{\u2022}$ | $\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-\mathrm{H}{\mathrm{O}}^{\u2022}+\mathrm{D}\mathrm{C}\mathrm{F}\stackrel{{\mathrm{k}}_{12}{}^{(\mathrm{h}\mathrm{e}\mathrm{t})(\mathrm{c})}}{\to}\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})+\mathrm{P}$ | (18) | |

${\mathrm{O}}_{3}{}^{-\u2022}+{\mathrm{H}}^{+}\stackrel{{\mathrm{k}}_{3}}{\to}\mathrm{H}{\mathrm{O}}^{\u2022}+{\mathrm{O}}_{2}$ | (3) | Catalyst Activation | |

Homogeneous attack of $\mathrm{H}{\mathrm{O}}^{\u2022}$ | $\mathrm{T}\mathrm{i}{\mathrm{O}}_{2}\stackrel{{\varphi}_{\mathrm{T}\mathrm{i}{\mathrm{O}}_{2}}}{\to}{\mathrm{e}}^{-}+{\mathrm{h}}^{+}$ | (19) | |

$\mathrm{H}{\mathrm{O}}^{\u2022}+\mathrm{D}\mathrm{C}\mathrm{F}\stackrel{{\mathrm{k}}_{4}}{\to}\mathrm{P}+\mathrm{H}{\mathrm{O}}_{2}{}^{\u2022}$ | (4) | Hole Trapping | |

Homogeneous propagation | $\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-\mathrm{O}{\mathrm{H}}^{-}+{\mathrm{h}}^{+}\stackrel{{\mathrm{k}}_{13}^{(\mathrm{h}\mathrm{e}\mathrm{t})}}{\to}\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-\mathrm{H}{\mathrm{O}}^{\u2022}$ | (20) | |

${\mathrm{O}}_{3}+\mathrm{H}{\mathrm{O}}^{\u2022}\stackrel{{\mathrm{k}}_{5}}{\to}\mathrm{H}{\mathrm{O}}_{2}{}^{\u2022}+{\mathrm{O}}_{2}$ | (5) | $\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-{\mathrm{H}}_{2}\mathrm{O}+{\mathrm{h}}^{+}\stackrel{{\mathrm{k}}_{14}{}^{(\mathrm{h}\mathrm{e}\mathrm{t})}}{\to}\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-\mathrm{H}{\mathrm{O}}^{\u2022}+{\mathrm{H}}^{+}$ | (21) |

$\mathrm{H}{\mathrm{O}}_{2}{}^{-}+\mathrm{H}{\mathrm{O}}^{\u2022}\stackrel{{\mathrm{k}}_{6}}{\to}\mathrm{H}{\mathrm{O}}_{2}{}^{\u2022}+\mathrm{O}{\mathrm{H}}^{-}$ | (6) | Electron Trapping | |

${\mathrm{O}}_{3}+\mathrm{H}{\mathrm{O}}_{2}{}^{-}\stackrel{{\mathrm{k}}_{7}}{\to}\mathrm{H}{\mathrm{O}}_{2}{}^{\u2022}+{\mathrm{O}}_{3}{}^{-\u2022}$ | (7) | $\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})+{\mathrm{e}}^{-}\stackrel{}{\rightleftarrows}\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{I}\mathrm{I})$ | (22) |

$\mathrm{H}{\mathrm{O}}_{2}{}^{\u2022}\underset{{\mathrm{k}}_{-8}}{\overset{{\mathrm{k}}_{8}}{\rightleftarrows}}{\mathrm{O}}_{2}{}^{-\u2022}+{\mathrm{H}}^{+}$ | (8) | $\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{I}\mathrm{I})+{\mathrm{O}}_{2}\to \mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-{\mathrm{O}}_{2}{}^{-\u2022}$ | (23) |

${\mathrm{O}}_{2}{}^{-\u2022}+{\mathrm{O}}_{3}\stackrel{{\mathrm{k}}_{9}}{\to}{\mathrm{O}}_{3}{{}^{-}}^{\u2022}+{\mathrm{O}}_{2}$ | (9) | $\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{I}\mathrm{I})+{\mathrm{O}}_{3}\stackrel{{\mathrm{k}}_{15}{}^{(\mathrm{h}\mathrm{e}\mathrm{t})}}{\to}\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-{\mathrm{O}}_{3}{}^{-\u2022}$ | (24) |

Adsorption processes | Pair Electron-Hole Recombination | ||

${\mathrm{O}}_{\mathrm{L}}{}^{2-}+\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})+{\mathrm{H}}_{2}\mathrm{O}\stackrel{}{\rightleftarrows}{\mathrm{O}}_{\mathrm{L}}{\mathrm{H}}^{-}+\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-\mathrm{O}{\mathrm{H}}^{-}$ | (10) ^{1} | ${\mathrm{e}}^{-}+{\mathrm{h}}^{+}\stackrel{{\mathrm{k}}_{16}}{\to}\mathrm{H}\mathrm{e}\mathrm{a}\mathrm{t}$ | (25) |

$\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})+{\mathrm{H}}_{2}\mathrm{O}\stackrel{}{\rightleftarrows}\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-{\mathrm{H}}_{2}\mathrm{O}$ | (11) | Homogeneous Photolysis | |

$\mathrm{S}+\mathrm{D}\mathrm{C}\mathrm{F}\stackrel{}{\rightleftarrows}\mathrm{D}\mathrm{C}\mathrm{F}-\mathrm{S}$ | (12) | ${\mathrm{O}}_{3}+{\mathrm{H}}_{2}\mathrm{O}\stackrel{{\varphi}_{{\mathrm{O}}_{3}}}{\to}{\mathrm{H}}_{2}{\mathrm{O}}_{2}+{\mathrm{O}}_{2}$ | (26) |

$\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-\mathrm{H}{\mathrm{O}}^{\u2022}\stackrel{}{\rightleftarrows}\mathrm{H}{\mathrm{O}}^{\u2022}+\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})$ | (13) | ${\mathrm{H}}_{2}{\mathrm{O}}_{2}+\mathrm{H}{\mathrm{O}}^{\u2022}\stackrel{{\mathrm{k}}_{17}}{\to}\mathrm{H}{\mathrm{O}}_{2}{}^{\u2022}+{\mathrm{H}}_{2}\mathrm{O}$ | (27) |

Initializing heterogeneous reaction | |||

$\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-\mathrm{O}{\mathrm{H}}^{-}+{\mathrm{O}}_{3}\stackrel{{\mathrm{k}}_{10}{}^{(\mathrm{h}\mathrm{e}\mathrm{t})}}{\to}\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-{\mathrm{O}}_{3}{}^{-\u2022}+\mathrm{H}{\mathrm{O}}^{\u2022}$ | (14) | ||

Propagation heterogeneous reaction | |||

$\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-{\mathrm{O}}_{3}{}^{-\u2022}+{\mathrm{H}}^{+}\stackrel{{\mathrm{k}}_{11}{}^{(\mathrm{h}\mathrm{e}\mathrm{t})}}{\to}\mathrm{T}\mathrm{i}(\mathrm{I}\mathrm{V})-\mathrm{H}{\mathrm{O}}^{\u2022}+{\mathrm{O}}_{2}$ | (15) |

Kinetic Constants | Computed Values | Reported Values | Error (%) | Units |
---|---|---|---|---|

${k}_{1}$ | $1.00\times 10$ | $6.00\times {10}^{8}$ | 99.99 | ${\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$ |

${k}_{2}$ | $3.00\times {10}^{-1}$ | $4.20\times {10}^{3}$ | 99.92 | ${\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$ |

${k}_{3}$ | $4.26\times {10}^{-2}$ | $3.12\times {10}^{12}$ | 100.00 | ${\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$ |

${k}_{4}$ | $1.15\times {10}^{-1}$ | $4.50\times {10}^{11}$ | 100.00 | ${\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$ |

${k}_{5}$ | $2.00\times {10}^{9}$ | $1.20\times {10}^{11}$ | 98.33 | ${\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$ |

${k}_{6}$ | $1.00\times {10}^{-4}$ | $4.50\times {10}^{11}$ | 100.00 | ${\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$ |

${k}_{7}$ | $7.66\times {10}^{-2}$ | $1.68\times {10}^{8}$ | 99.99 | ${\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$ |

${k}_{8}$ | $1.45\times {10}^{4}$ | $4.74\times {10}^{7}$ | 99.97 | ${\mathrm{min}}^{-1}$ |

${k}_{-8}$ | $3.28\times {10}^{9}$ | $1.20\times {10}^{12}$ | 99.73 | ${\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$ |

${k}_{9}$ | $1.97\times {10}^{6}$ | $9.60\times {10}^{10}$ | 99.99 | ${\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$ |

Kinetic Constants | Computed Values | Units |
---|---|---|

${k}_{10}^{(het)}$ | $3.04\times {10}^{4}$ | ${\mathrm{L}}^{2}\mathrm{m}\mathrm{o}{\mathrm{l}}^{-1}{\mathrm{m}}^{-2}{\mathrm{min}}^{-1}$ |

${k}_{11}^{(het)}$ | $3.62\times {10}^{8}$ | ${\mathrm{L}}^{2}\mathrm{m}\mathrm{o}{\mathrm{l}}^{-1}{\mathrm{m}}^{-2}{\mathrm{min}}^{-1}$ |

${k}_{12}^{(het)}$ | $3.19\times {10}^{-2}$ | ${\mathrm{L}}^{2}\mathrm{m}\mathrm{o}{\mathrm{l}}^{-1}{\mathrm{m}}^{-2}{\mathrm{min}}^{-1}$ |

Kinetic Constants | Computed Values | Reported Values | Error (%) | Units |
---|---|---|---|---|

${\varphi}_{Ti{O}_{2}}$ | $3.22\times {10}^{-3}$ | – | – | $\mathrm{m}\mathrm{o}\mathrm{l}\mathrm{E}\mathrm{i}\mathrm{n}\mathrm{s}\mathrm{t}\mathrm{e}\mathrm{i}{\mathrm{n}}^{-1}$ |

${k}_{13}^{(het)}$ | $3.55\times {10}^{-4}$ | – | – | ${\mathrm{L}}^{2}\mathrm{m}\mathrm{o}{\mathrm{l}}^{-1}{\mathrm{m}}^{-2}{\mathrm{min}}^{-1}$ |

${k}_{14}^{(het)}$ | $2.05\times {10}^{-3}$ | – | – | $\mathrm{L}{\mathrm{m}}^{-2}{\mathrm{min}}^{-1}$ |

${k}_{15}^{(het)}$ | $7.20\times {10}^{-2}$ | – | – | ${\mathrm{L}}^{2}\mathrm{m}\mathrm{o}{\mathrm{l}}^{-1}{\mathrm{m}}^{-2}{\mathrm{min}}^{-1}$ |

${k}_{16}^{(het)}$ | $3.60\times {10}^{-4}$ | – | – | ${\mathrm{L}}^{2}\mathrm{m}\mathrm{o}{\mathrm{l}}^{-1}{\mathrm{m}}^{-2}{\mathrm{min}}^{-1}$ |

${\varphi}_{UV}$ | $2.10\times {10}^{-1}$ | – | – | ${\mathrm{min}}^{-1}$ |

${k}_{17}$ | $1.07\times {10}^{12}$ | $1.62\times {10}^{9}$ | $>100.00$ | ${\mathrm{M}}^{-1}{\mathrm{min}}^{-1}$ |

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