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Ultrasound enhancement of near-neutral photo-Fenton for effective E. coli inactivation in wastewater

Giannakis, Stefanos,Papoutsakis, Stefanous,Darakas, Efthymios,Escalas Cañellas, Antoni,Petrier, Christian,Pulgarin, César

Abstract

In this study, we attempt for the first time to couple sonication and photo-Fenton for bacterial inactivation of secondary treated effluent. Synthetic wastewater was subjected to sequential high-frequency/low power sonication, followed by mild photo-Fenton treatment, under a solar simulator. It was followed by the assessment of the contribution of each component of the process (Fenton, US, hv) towards the removal rate and the long-term survival; sunlight greatly improved the treatment efficiency, with the coupled process being the only one to yield total inactivation within the 4-h period of treatment. The short-term beneficial disinfecting action of US and its detrimental effect on bacterial survival in long term, as well as the impact of light addition were also revealed. Finally, an investigation on the operational parameters of the process was performed, to investigate possible improvement and/or limitations of the coupled treatment; 3 levels of each parameter involved (hydraulic, environmental, US and Fenton) were tested. Only H2O2 increased improved the process significantly, but the action mode of the joint process indicated potential cost-effective solutions towards the implementation of this method. (C) 2014 Elsevier B.V. All rights reserved.

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1  Ultrasound enhancement of near-neutral photo-Fenton for effective E. coli 1 inactivation in wastewater 2 3 Stefanos Giannakis1,2,3, Stefanos Papoutsakis3, Efthymios Darakas1, Antoni Escalas-4 Cañellas2,4, Christian Pétrier5,6, César Pulgarin3,* 5 1Laboratory of Environmental Engineering and Planning, Department of Civil Engineering, Aristotle University of 6 Thessaloniki, 54624 Thessaloniki, Greece 7 2Laboratory of Control of Environmental Contamination, Institute of Textile Research and Industrial Cooperation of Terrassa 8 (INTEXTER), Universitat Politècnica de Catalunya, Colom 15, 08222 Terrassa, Catalonia, Spain 9 3Swiss Federal Institute of Technology, Lausanne, Institute of Chemical Sciences and Engineering, 1015 Lausanne, 10 Switzerland 11 4Department of Chemical Engineering & Terrassa School of Engineering, Universitat Politècnica de Catalunya, Colom 1, 12 08222, Terrassa, Catalonia, Spain 13 5Laboratoire Rhéologie et Procédés, Grenoble-INP, UMR CNRS 5520, BP 53, 38041 Grenoble Cedex 9, France 14 6King AbdulAziz University, Jeddah, Saudi Arabia 15 *Corresponding author: César Pulgarin, Tel: +41216934720; Fax: +41216936161; E-mail: 16 [email protected] 17 18 Abstract 19 In this study, we attempt for the first time to couple sonication and photo-Fenton for bacterial 20 inactivation of secondary treated effluent. Synthetic wastewater was subjected to sequential high-21 frequency/low power sonication, followed by mild photo-Fenton treatment, under a solar simulator. It 22 was followed by the assessment of the contribution of each component of the process (Fenton, US, hv) 23 towards the removal rate and the long-term survival; sunlight greatly improved the treatment 24 efficiency, with the coupled process being the only one to yield total inactivation within the 4-h period 25 of treatment. The short-term beneficial disinfecting action of US and its detrimental effect on bacterial 26 survival in long term, as well as the impact of light addition were also revealed. Finally, an 27 investigation on the operational parameters of the process was performed, to investigate possible 28 improvement and/or limitations of the coupled treatment; 3 levels of each parameter involved 29 (hydraulic, environmental, US and Fenton) were tested. Only H2O2 increased improved the process 30 significantly, but the action mode of the joint process indicated potential cost-effective solutions 31 towards the implementation of this method. 32 Keywords: wastewater disinfection, photo-Fenton, high-frequency ultrasound, E. coli, inactivation 33 mechanism34 NOTICE:thisistheauthor’sversionofaworkthatwasacceptedforpublicationinUltrasonicsSonochemistr y .Changesresultingfromthepublishingprocess,suchas peerreview,editing,corrections,structuralformatting,andotherqualitycontrolmechanismsmaynotbereflectedinthisdocument.Changesmayhavebeenmadeto thisworksinceitwassubmittedforpublication.AdefinitiveversionwassubsequentlypublishedinUltrasonicsSonochemistry[Vol.22,p.515‐526,January2015].DOI: 10.1016/j.ultsonch.2014.04.015 2  1. INTRODUCTION 35 36 Advanced Oxidation Processes (AOPs) have been in the spotlight for more than three decades, as part 37 of a global effort to modernize actual methods of water disinfection. Their action is based on the 38 production of the extremely oxidizing hydroxyl radical (•OH) [1], which can attack the chemical 39 structure of the microorganisms’ cell wall and inactivate them [2]. Ultrasound has been extensively 40 studied as an AOP, targeting microorganism inactivation, such as bacteria, viruses etc., by either low 41 (~20 kHz) or high frequencies (200+ kHz) [2, 3, 4 and 5]. This method is exploiting the direct 42 mechanical action of the cavitation bubble implosion (low frequencies) as well as the additional 43 production of H2O2 and •OH radicals during cavitation (high frequencies); the propagation of 44 ultrasound waves in the aqueous medium initiates the aforementioned actions, by the generation of 45 extreme temperature and pressure conditions [6], which have a proven bactericidal effect [7, 8, 9, and 46 10]. 47 As far as the ultrasound set-up is concerned, the frequency of the ultrasonic waves is a crucial 48 parameter, for it defines the size of the cavitation bubbles [11]. Literature suggests that the average 49 cavity size is proportional to the acoustic power and inversely proportional to the ultrasound frequency 50 [12]. It is also verified that apart from low frequency/high power ultrasound systems [13, 14], high 51 frequency/low power processes have been proven to efficiently inactivate microorganisms [8, 15, and 52 16]. However, ultrasound already requires high intensities to achieve total inactivation of 53 microorganisms, and therefore, is considered an expensive application for large volumes of water [2]. 54 Considering all the above, it should be used preferably as a complementary disinfecting method [2]. 55 The photo-Fenton process [17] could play the role of the main disinfecting method, as one of the most 56 efficient methods of hydroxyl radical production [18]. Lately, it has even been used to disinfect 57 drinking water, being a good alternative to chlorination, with its known disinfection by-products 58 formation [19]. However, wastewater is a complex matrix in which many organic and inorganic 59 compounds coexist, such as nutrients, salts and many substances that could influence the outcome of 60 the application of either process. It has been reported that the presence of hydroxyl radical scavengers, 61 namely the organic matter, presents an additional oxidation target and renders AOPs sensitive to the 62 treatment of wastewater [20, 21]. Suppression of these scavengers revealed their importance [10] and 63 also, for years the Fenton reaction was believed to be a pH-restricted reaction in highly acidic regions; 64 it was considered impossible to apply such methods, in matrices with near-neutral pH [22]. However, 65 recent advances [18, 23 and 24] have proven its effectiveness in the neutral area, and in the 66 simultaneous presence of organic matter [18, 25]. Previous work in our group has shown, there is no 67 need for acidification prior to the treatment to keep a significant part of the iron soluble; apart from the 68 direct complexion with bacteria, there are some strong photoactive Fe3+ complexes formed in presence 69 of organic matter [21, 25]: 70 3  [R-COO- - Fe3+]2+  hv  Fe2+ + CO2 + R• (1) 71 The cycle continues with the reaction of the regenerated iron with hydrogen peroxide to produce more 72 hydroxyl radicals etc. 73 Fe2+ + H2O2  OH- + •OH + Fe3+ (2) 74 In order to increase the amount of water treated by solar-assisted methods, compound parabolic 75 collector reactors have been used [17, 18, 23 and 26], and solar photo-Fenton even was a subject under 76 question, because of the intermittent action of the light [27]. There is a technical issue to be addressed 77 in the intermittent nature of this treatment method, and the existence of “dead” time among the 78 experiment. Typically, a CPC photo-reactor consists of the illuminated surface and the storage-79 recirculation tank. The recirculating flow of these reactors creates a gap in the illumination for as long 80 as water is present in the (dark) storage tank, allowing bacterial defense mechanisms to deploy [28]. 81 Literature indicates a variety of light-to-dark distributions (Table 1), which materialize this difference 82 [17, 18, 23, 26, 29, 30 and 31]. 83 Therefore, keeping in mind the improvement of the near-neutral photo-Fenton disinfection while 84 working within realistic operational parameters, for the first time we study the joint ultrasound/photo-85 Fenton treatment for wastewater, in a CPC-like, lab-scale system. In this manner, we will take 86 advantage of two factors that could work complementing each other: firstly, the exploitation of the 87 dark intervals for sonication, along with the utilization of solar energy for the promotion of a mild 88 photo-Fenton reaction and secondly, the supplementary action these processes have, since, for 89 instance, US can produce H2O2 and subsequently, could fuel the photo-Fenton process. In our study, 90 synthetic secondary effluent was used, spiked with E. coli K12, recirculating around a sonicated dark 91 reactor and an illuminated batch reactor, under solar simulated light. We aim to: 92 i) Explore the effects of the photo-Fenton factors (light, reactants) and the ultrasonic action 93 (US) on both short and long-term disinfection events; clarification of the effects is 94 attempted by stepwise insertion of the participating actions. 95 ii) Investigate the involved operational parameters (recirculation speed, temperature, light 96 intensity, treated volume and distribution of volumes, iron and hydrogen peroxide content, 97 ultrasound intensity) in a small-scale set-up. 98 99 2. MATERIALS AND METHODS 100 101 2.1. Synthetic secondary effluent preparation 102 103 4  2.1.1. Microbial methods 104 The E. coli strain K12 (MG1655) employed was provided by the “Deutsche Sammlung von 105 Mikroorganismen und Zellkulturen”. Luria-Bertani broth was inoculated with a colony from bacterial 106 E. coli pre-cultures, placed in 50 ml plastic falcons for 8 h and then loop inoculated, after 1% dilution 107 overnight (180 rpm and 37°C for 15 h), to achieve stationary phase cells. 108 Harvested cells were centrifuged and washed three times (5000 rpm, 15 and 5 min for separation and 109 washing, respectively), followed by reservation in saline solution (neutral pH solution with 8 g/L NaCl 110 and 0.8 g/L KCl); a solution of 109 CFU/mL is achieved. 111 112 2.1.2. Synthetic wastewater composition 113 The preparation of the synthetic wastewater took place as under the directive of SYMAWE [32]. The 114 initial DOC was 100 mg/L (250 mg/L COD). The experiments used a 10% dilution (in distilled water) 115 of the said composition. The dilution performed corresponds to the COD and DOC values encountered 116 in normal secondary effluents. Finally, the pH of the sample was between 6.5-7. 1 mL of the prepared 117 bacterial solution was used to spike the diluted wastewater, thus resulting in an initial bacterial 118 population of 106 CFU/mL. 119 120 2.2. Reagents and analyses 121 122 The wastewater constituents, as well as the Fenton reagents were used as received. Photo-Fenton 123 experiments were carried out employing ferrous sulfate heptahydrate (Fluka Chemika), hydrogen 124 peroxide (35% by weight, Sigma Aldrich), used as received. The dissolved iron (Fe2+, Fe3+) was 125 measured with the ferrozine method [33], using a UV-Vis Lambda 20 spectrophotometer, provided by 126 PerkinElmer, Schwerzenbach, Switzerland. For 1.6 mL of sample 0.2 of ferrozine solution (4.9 mM) 127 was added, followed by 0.2 mL of hydroxylamine hydrochloride solution 10% w/w. Acetate buffer 128 solution was added for a final 4.5-5 pH value. To determine the concentration of hydrogen peroxide in 129 the sample titanium oxysulfate solution was added, also measured with the same spectrophotometer. 130 The pH of each sample was measured with a pH-meter provided by Mettler Toledo (PH/Ion S220, 131 Seven Compact, Mettler Toledo). 132 133 2.3. Description of reactors’ set-up 134 135 The preliminary study was carried out in plain Pyrex glass batch reactors of 65 mL total capacity. In 136 the set-up presented in Figure 1, the configuration permits the sequential treatment of the synthetic 137 5  wastewater; US/photo-Fenton treatment was taking place (or vice versa). The same configuration was 138 used in one of our previous works, (used in [29], similar to the set-up used by Mendez-Arriaga et al, 139 2009 [34]), synthetic wastewater from a cylindrical double-wall glass vessel (400 mL) was pumped by 140 a peristaltic pump through three glass reactors (diameter 3.8 cm, effective irradiation surface 214.8 141 cm2), connected in series, of total volume 230 mL. Temperature was regulated by water recirculating 142 around the reactor and connected to a thermostat. The third reactor effluent was recirculated to the 143 original vessel. Normally, water was inserted in the double-wall reactor and pumped into the irradiated 144 part. Therefore, 230 mL of water were always present under illumination, 70 mL in the distribution 145 system and the rest subjected to sonication. 146 The ultrasonic waves (275 kHz) were emitted from a piezoelectric 4-cm disc, fixed on a Pyrex glass 147 plate adjusted to the bottom of the double-walled reactor. The intensities applied in all experiments 148 were 10, 20 and 40 W. The electric power was the chosen method to calibrate the ultrasonic 149 equipment. The in-series reactors were irradiated by the Suntest apparatus. The Suntest CPS solar light 150 simulator bears a lamp that emits ~0.5% of the photons at wavelengths <300 nm, ~7% between 300 151 and 400 nm and the rest follow the solar spectrum. The global irradiance values used in this work were 152 800, 1000 and 1200 W/m2, while the corresponding UV values were approximately 19.2, 24.7 153 and 30.2 W/m2. 154 155 2.4. Experimental design 156 157 Two sets of experiments were performed. In a first set of 8 experiments, that we call step-wise 158 construction of the joint treatment process, the elements of the US/hv/Fe/H2O2 were gradually and 159 accumulatively applied to the wastewater, in order to determine the individual role of each factor and 160 to detect any synergy among them. Table 2 shows the conditions corresponding to each individual 161 treatment factor when applied. Table 3 summarizes the four subsets of experiments in the step-wise 162 design. 163 In a second set of experiments (improvement of the process efficiency), eight different variables were 164 individually modified at three levels, while keeping the other variables constant, in order to obtain 165 improved working levels for each variable. Table 4 displays the three values (levels) essayed for each 166 variable. In each experiment the remaining parameters were kept constant and set to the central value 167 shown in the table. 168 169 2.5. Bacterial enumeration and regrowth tests 170 171 6  The disinfection efficiency was measured by viable plate counts on Petri dishes containing PCA agar 172 (plastic, 9-cm diameter). The pour-plating method was used and dilutions were made to ensure 173 countable numbers on the plates, i.e. 20-100 colonies/plate. Experiments were performed twice and 174 plating took place in 2-3 consequent dilutions and in duplicates. 175 Regrowth of bacteria was estimated after the storage of the samples at ambient temperature for 24 and 176 48 h after the sampling time. Samples were kept in 1.5 mL plastic Eppendorf caps in the dark and the 177 population was measured to assess the post-irradiation events, after their removal from the 178 experimental set-up. 179 180 3. RESULTS AND DISCUSSION 181 182 3.1. Results of the step-wise construction of the joint treatment process 183 184 As far as a potential application of mild photo-Fenton assisted by high frequency/low power 185 ultrasound is concerned, moderate concentrations of reactants are suggested for the evolution of our 186 study, after an initial investigation (data not shown). At 1000 W/m2 light intensity, an addition of 1 187 ppm iron and 10 ppm of H2O2 will be used, as marginal values of Fenton reagents and 20 W of US 188 power. 189 190 3.1.1. Disinfection efficiency 191 192 i) Experiments: 1-2 (WW and WW/Fe/H2O2). 193 Figure 2a presents the results of the first part of the experiments, where neither light nor US was 194 applied. Wastewater was recirculated around the non-illuminated, non-sonicated experimental set-up 195 and the corresponding graphs describe the changes when H2O2 and iron were added to the solution. 196 We notice the increase of the population, when no reactants were added, due to the existence of 197 nutrients and salts that favor bacterial growth in this water matrix [35]. H2O2 is a substance with 198 disinfecting action, while iron itself is not toxic for bacteria. The addition of both reactants causes the 199 initiation of the Fenton reaction, which has a slow, but existing disinfecting ability and within a 200 timeframe of 4 h, we observe a 24.4% reduction in the initial population. 201 202 ii) Experiments: 3-4 (US and US/Fe/H2O2). 203 7  Figure 2b demonstrates the effects sonication has on samples, alongside with the stepwise insertion of 204 the Fenton reagents. The sample recirculates around the ultrasound vessel and the non-illuminated 205 area, being subject to intermittent high-frequency, low intensity sonication. When ultrasound alone is 206 applied, there is a decrease in total bacterial numbers, approaching 27.9%. The concurrent addition of 207 both Fenton reactants (H2O2 and Fe2+) in the sonicated sample causes an 82.1% reduction in the 208 bacterial population, compared to 27.9 % reduction for US treatment and 24.4% for Fenton treatment 209 alone. This indicates a synergy between sonication and the Fenton reagents; a synergy factor of 1.57 is 210 demonstrated by the disinfecting efficiency of the reactions. 211 During sonication, the breakage of the cavitation bubbles can lead to the formation of an almost point-212 sized heat source [36, 37], with local temperatures approaching 2000 K and pressures of 200 atm. 213 These extreme conditions can cause lysis of water molecules and along with that, extra production of 214 hydroxyl radicals [8]. The presence of the afore-mentioned particles in real wastewater and the 215 bacteria (in our matrix) could also play another important role, since the collapse of the cavitation 216 bubbles near a particle in the medium could cause micro-jets, depending on the size of the particle [38] 217 and could also form “weak spots” in the body of the liquid; these are potential places to form a cavity 218 [39]. It has been also reported that the presence of some salts causes a baro-protective effect on the 219 cells [40] and samples with higher contents of soluble solids would require higher sonication times. 220 Apart from the physical damage, during the ultrasound treatment of the sample, there is ample 221 generation of reactive oxygen species (•OH radicals [41], singlet oxygen [42, 43]), as mentioned 222 before, which are known to stress bacteria and lead to cell death [25, 44]. 223 Finally, the addition of peptone (present in the synthetic wastewater) and the generally, presence of 224 nitrogen compounds has been reported to delay the sonicated degradation of phenols [45]. However, 225 nitrogen, under the presence of ultrasound waves can form NOx (nitrate and nitrite). Its reaction with 226 singlet oxygen (as produced before) [43] produces peroxynitrite (ONOO-) [46]. Peroxynitrite is 227 included in the reactive nitrogen species and can cause significant injures to various structures of the 228 cell (free radical damage or attack against the respiratory chain) [46]. 229 The synergistic action of US and Fenton processes can be attributed to the exploitation of the 230 recombined H2O2 (from •OH), which is less oxidative than the hydroxyl radical itself, and with that, the 231 re-initiation of the Fenton reaction with new reactants. Also, the ultrasound process, according to 232 Kryszczuk [47], increases the transient breakage of the bonds among the molecular components of the 233 cell membrane, which increases the permeability of the cell in external substances [48]. Therefore, the 234 introduction of Fe2+ in the cell is easier and its presence inside the cell can produce hydroxyl radicals 235 very close to vital functions of the cell, as well as the DNA [25] due to the induced internal Fenton 236 process. 237 238 iii) Experiments: 5-6 (hv and hv/Fe/H2O2). 239 8  The 3rd set of experiments is dedicated in the investigation of the impact of light in the sequential 240 process. In all experiments light is provided at 1000 W/m2, but in total, intermittent irradiation is 241 provided to the system; there is an illuminated regime and a non-illuminated one, in the Suntest 242 apparatus and the (inactive) sonication vessel (and tubing). In one of our previous works [29], we 243 demonstrated the impact light intermittence has on bacterial disinfection and survival, while 244 continuous supply or very fast recirculation around illuminated and dark regimes favors disinfection, 245 with the same set-up. Therefore, photo-Fenton is promoted in non-intermittent regimes or, as in our 246 case, short dark interval periods. 247 As it can be seen from Figure 2c, light, even in non-continuous form, is very effective and results in 248 high inactivation rates. Its disinfecting action is dominating the removal process, until the Fenton 249 reagents are present, and solar-assisted photo-Fenton is induced. The action of photo-Fenton is taking 250 place within the Suntest and dark (normal) Fenton takes place during the rest of the time, in a 0.85:1 251 time distribution (46% photo-Fenton over 54% Fenton). After an initial delay, which is demonstrated 252 as a shoulder in the graph, reaction is more effective by the hv/Fe/H2O2 than the corresponding solar 253 treatment. 254 Spuhler et al. [25] have reviewed the mechanism of bacterial inactivation by the photo-Fenton reaction 255 in near-neutral water with organic components, and have suggested the possible sources of ROS 256 production and cellular photo-oxidative damage, as well as the damage done by the ROS themselves, 257 deriving from the photo-Fenton reaction. In our suggested treatment method, these mechanisms are 258 completely compatible, explaining the majority of the actions and other works on near-neutral photo-259 Fenton mechanisms describe fully the mechanisms, so we will not further analyze their findings. 260 261 iv) Experiments: 7-8 (hv/US and hv/US/Fe/H2O2). 262 The final group of experiments are presented in Figure 2d. This graph summarizes the results of the 263 joint treatment by light and ultrasound. It is clear, after a comparison with Figure 2c, that when light is 264 present, its disinfecting action is dominating the process. However, we observe that the only case total 265 disinfection is achieved, is by the sequential US/pF system. In this system, wastewater spends its time 266 distributed 46% under photo-Fenton, 14% in the dark (dark-Fenton) and 40% in the sonication vessel 267 (US/Fenton). The experimental time has less inactive periods, and we observe that it has a significant 268 impact in the total inactivation of the bacterial populations in less than 4h. Here, the photo-Fenton/US 269 synergy is low in terms of bacterial counts, efficiency was improved in a relatively low percentage, but 270 only the coupled process resulted in total disinfection in 4 h. The elevated efficiency and total 271 inactivation for the first time, is attributed to the combination of all the previous actions (in US and/or 272 light), as well as the following actions (a graphical summary of all the actions is presented in Figure 273 3): 274 9  i. The hydroxyl radical is a short living ROS, and it occurs not to reach the target in all cases and 275 often recombines to create H2O2 [49]. Therefore, the addition of ultrasound directly produces 276 hydroxyl radicals and H2O2; the •OH directly attacks the cell and H2O2 participates in the 277 photo-Fenton reaction (2). Alongside with the added H2O2, there is additional production, 278 fueling the Fenton reaction and thus, improving the overall efficiency of the treatment. 279 ii. As we described before, with ultrasound waves, the loosening of transient bonds and insertion 280 of Fe2+ in the cell is increased, which promotes the internal Fenton reaction. After the 281 completion of the Fenton reaction, light reduces Fe3+ to Fe2+, and re-initiates a radical 282 production inside the cell (internal photo-Fenton). 283 iii. Low frequency ultrasound has been proven [50] to reduce Fe3+ in the form of ferrous ions 284 (Fe2+). The average size of the bubble however decreases when frequency is increased, in our 285 system [12]; nevertheless, cavitation still takes place. Therefore, it is possible that an action 286 like this could provide an additional source of iron available for the photo-Fenton process, and 287 progress the regeneration of the catalyst in the (otherwise) non-illuminated part of the time. In 288 that way, more available ferrous ions can be present in the solution. 289 iv. We mentioned the extreme temperature and pressure conditions that take place during the 290 collapse of the cavitation bubbles. The interior part of the bubble, under these conditions, is 291 known to emit light, under the phenomenon of sono-luminescence [8]. The optical aspects of 292 this phenomenon have been studied [51] and the emitted light wavelengths fall into the 293 necessary ones possibly able i) to induce the regeneration of the photo-Fenton reaction 294 catalyst, ii) inflict direct UV damage to the cell. However, the necessary energy to achieve this 295 is still under question. 296 v. Apart from the radicals’ production through the normal photo-Fenton cycle, the presence of 297 light is participating in another series of reactions with nitrogen compounds. The photolysis of 298 nitrate and nitrites (produced by the participation of the US in the process) can lead to 299 additional hydroxyl radical production [45]: 300 Photolysis of Nitrate: 301  →    (3) 302  →      (4) 303    ↔    (5) 304 Photolysis of Nitrite: 305  →     (6) 306    ↔    (7) 307 308 16  Swiss Government for the Swiss Government Excellence Scholarship, by means of which Stefanos 518 Giannakis has received a Research Visit fellowship (No. 2012.0499). Finally, Stefanos Papoutsakis 519 was funded by the Swiss-Hungarian Co-operation Program “Sustainable fine chemical, 520 pharmaceutical industry: screening and utilization of liquid wastes – Innovative approaches for the 521 abatement of industrial/toxic waste in aqueous effluents”. 522 523 6. REFERENCES 524 525 1. I. Oller, S. Malato, J.A. Sánchez-Pérez, W. Gernjak, M.I. Maldonado, L.A. 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(2009) 20 14 0.70 32% 68% 0.47 MoncayoLasso et al. (2009) 17.5 20 1.14 45% 55% 0.82 FernandezIbañez et al. (2005) (varied flowrates) 5, 13, 22.5 11 2.2, 0.85, 0.49 49% 51% 0.96 Rincon & Pulgarin (2007) (min, max capacity) 20.5 37, 70 1.80, 3.41 65%, 34% 35%, 66% 1.86, 0.52 Sciacca et al. (2011) 24.2 18 0.74 83% 17% 4.88 Giannakis et al. (2013) 0.03, 0.06, 0.07 0.7 22.58, 12.28, 9.59 33% 67% 0.49 Ndounla et al. (2013) 2 25 12.5 60% 40% 1.53 698 Table 2 – Parameters involved in the joint treatment process 699 Factors Values Other parameters Light 1000 W/m2Temperature: 30˚C Ultrasound 20 W Recirculating Flow rate: 4.39 L/h Iron 1 ppm Treated Volume: 500 mL H2O2 10 ppm Initial Population: 106 CFU/mL 700 701 21  Table 3 – Subsets of experiments in the step-wise construction of the joint hv/US/Fe/H2O2 702 treatment process. 703 Experiments Treatment constituents 1-2 WW and WW/Fe/H2O2 ‐ Wastewater with no treatment ‐ Wastewater + Fe/H2O2 3-4 US and US/Fe/H2O2 ‐ Wastewater+US ‐ Wastewater+US+Fe/H2O2 5-6 hv and hv/Fe/H2O2 ‐ Light ‐ Light+/Fe/H2O2 (photo-Fenton) 7-8 hv/US and hv/US/Fe/H2O2 ‐ Light+US ‐ US+photo-Fenton 704 Table 4 – Overview of the investigation of the operational parameters 705 Factors1 Level 1 Level 2 Level 3 Hydraulic Pump rpm 33 66 99 No. of Illuminated vessels 1 2 3 Wastewater volume (mL) 500 600 700 Environmental Temperature (˚C) 10 20 30 Light Intensity (W/m2) 800 1000 1200 Fenton / Ultrasound H2O2 Concentration (ppm) 5 10 20 Fe Concentration (ppm) 0.5 1 2 US Acoustic Power (W) 10 20 40 1Central values are annotated with bold. 706 707 22  708 Table 5 – Hydraulic calculations on the reactor set-up 709 710 Increasing recirculation speed from 33 to 99 rpm (1.87 to 4.39 L/h) Reactors333rpmReactors366rpmReactors399rpm 23  711 Volume500mL1.87L/h1.87L/hVolume500mL3.44L/h3.44L/hVolume500mL4.39L/h4.39L/h Light230mL7.38min46%Light230mL4.01min46%Light230mL3.14min46% Tubing70mL2.25min14%Tubing70mL1.22min14%Tubing70mL0.96min14% US200mL6.42min40%US200mL3.49min40%US200mL2.73min40% Total500mL16.04min100%Total500mL8.72min100%Total500mL6.83min100% Increasing illuminated volume from 1 reactor to 3 (75 to 230 mL) Reactors199rpmReactors299rpmReactors399rpm Volume500mL4.39L/h4.39L/hVolume500mL4.39L/h4.39L/hVolume500mL4.39L/h4.39L/h Light75mL1.03min15%Light150mL2.05min30%Light230mL3.14min46% Tubing50mL0.68min10%Tubing60mL0.82min12%Tubing70mL0.96min14% US375mL5.13min75%US290mL3.96min58%US200mL2.73min40% Total500mL6.83min100%Total500mL6.83min100%Total500mLmL6.83min100% Increasing total treated volume from 500 to 700 mL Reactors399rpmReactors399rpmReactors399rpm Volume500mL4.39L/h4.39L/hVolume600mL4.39L/h4.39L/hVolume700mL4.39L/h4.39L/h Light230mL3.14min46%Light230mL3.14min38%Light230mL3.14min33% Tubing70mL0.96min14%Tubing70mL0.96min12%Tubing70mL0.96min10% US200mL2.73min40%US300mL4.10min50%US400mL5.47min57% Total500mL6.83min100%Total600mL8.20min100%Total700mL9.57min100% 24  List of Figures 712 713 Figure 1 – Experimental set-up, consisting of the illuminated area (Suntest apparatus), the recirculation pump, 714 the (dark) sonication vessel and the temperature control (thermostat). The flow direction is clockwise, water is 715 introduced at surface level and sampled from the bottom of the vessel. 716 717 718 Figure 2 – Experimental results from the coupling of photo-Fenton and sonication. a) Experiments 1-2 (WW and 719 WW/Fe/H2O2), b) Experiments 3-4 (US and US/Fe/H2O2), c) Experiments 5-6 (hv and hv/Fe/H2O2) and d) 720 Experiments 7-8 (hv/US and hv/US/Fe/H2O2). e) Long-term inactivation events for 48 h (time axis initiates in the 721 4-h mark, after treatment). 722 723 25  724 Figure 3 – Suggestion of the added actions sonication has towards bacterial inactivation, when coupled with 725 photo-Fenton. The known photo-Fenton mechanisms suggested by literature are not displayed. 726 727