22nd International Symposium on Plasma Chemistry July 5-10, 2015; Antwerp, Belgium Abatement of trichloroethylene by combined use of non-thermal plasma and CeO 2 S. Sultana1, A.M. Vandenbroucke1, M. Mora2, C. Jiménez-Sanchidrián2, F.J. Romero-Salguero2, C. Leys1, N. de Geyter1 and R. Morent1 1 Research Unit Plasma Technology (RUPT), Department of Applied Physics, Faculty of Engineering and Architecture, Ghent University, Belgium 2 Department of Organic Chemistry, Faculty of Sciences, University of Cordoba, Spain Abstract: This study is devoted to investigate the opportunities of a plasma-catalytic system with CeO 2 downstream (i.e., PPC-Post Plasma-catalysis) for the abatement of trichloroethylene from dry air. A multi-pin-to-plate negative DC corona/glow discharge is used and showed poor CO x selectivity despite having high abatement efficiency, when operated alone. Nonetheless, NTP enables catalyst activation at lower temperature. As a result, complete suppression of unwanted chlorinated by-products as well as high CO x selectivity at lower energy cost have been achieved. Keywords: non-thermal plasma, plasma-catalysis, trichloroethylene, cerium oxide 1. Introduction Air quality issues have become a huge concern of environmental legislation as a consequence of growing awareness in our global world. Air pollution is a mixture of natural and man-made substances in the air because of industrialization and transportation, which has repercussions on public’s health and on phenomena like acidification and eutrophication of the environment. Among these harmful pollutants, volatile organic compounds (VOCs) are the cardinal candidates which cause severe damage on human health due to their potential toxicity, carcinogenicity and mutagenicity [1]. Furthermore, they are also responsible for odour nuisance, the creation of tropospheric ozone leading to photochemical smog, the intensification of global warming and the depletion of stratospheric ozone layer [2]. Non-thermal plasma (NTP) technology has attracted growing interest of scientists over last two decades due to their distinctive characteristic of being able to provide a highly chemical reactive environment (e-, O*, HO 2 *, OH*, N 2 *, O 3 , ....) to decompose VOC at ambient condition which repudiates the use of expensive vacuum system [3, 4]. Although other commercial pollution control techniques (thermal incineration, catalytic oxidation or adsorption) are very efficient in VOC’s oxidation, these are energetically expensive and difficult to operate in case of moderate flow rates with low VOC concentration. In NTP, energetic electrons (1 - 10 eV) are produced consuming almost all the electric energy supplied to the system instead of heating entire gas unlike thermal and catalytic oxidation. Collision of these highly energetic electrons with neutral background molecules close to room temperature, generate active species such as free radicals, metastables, ions and secondary electrons through different chemical processes such as dissociation, O-3-6 excitation, and ionization. These active species are able to decompose pollutant molecules to less harmful Additionally, the products (CO 2 , H 2 O, HX, X 2 ). abatement of low concentrated VOC’s (up to 1000 ppm), feasible to indoor air treatment application, is challenging for conventional methods because when VOC’s concentration decreases, the cost per unit pollutant treatment becomes higher in comparison to NTP. Unfortunately, industrial implementation of NTP for VOC abatement is impaired by three main bottlenecks such as poor product selectivity, formation of undesired by-products that often increase the overall toxicity of the treated gas stream and low energy efficiency. In order to overcome these limitations many attempts have been made and engendered the development of a hybrid system using multiple techniques. During the last decade researchers have persistently been investigating a novel technique which combines the advantage of rapid ignition from NTP and high selectivity from catalyst, leading to increased energy efficiency and supressed unwanted by-products distribution for VOC decomposition. In such a hybrid system, the catalyst can be integrated either inside (IPC-Inside Plasma Catalysis) [5] or downstream (PPC-Post Plasma Catalysis) [6, 7] of discharge region, in both cases a synergetic effect has been reported in many studies [8-10]. The objective of this current work is to abate trichloroethylene (TCE) from dry air by combined use of multi-pin-to-plate negative DC corona/glow discharge with CeO 2 catalyst downstream. In order to minimize the energy cost of the abatement, combination of low energy density plasma and moderate catalyst temperature have been examined. 1 2. Experimental The experimental set-up was described in detail elsewhere [11] (Fig. 1). In brief, the plasma source consists of 10 aligned cathode pins (separated by 28 mm) and a single anode plate as counter electrode forming a rectangular duct (40 mm x 9 mm cross section and 400 mm length). The inter electrode gap in this configuration is 10 mm. A DC power supply (Technix, SR40-R-1200) is used to generate glow discharge at ambient conditions. The discharge voltage and current were varied between 8.0 - 10.5 kV and 0.04 - 0.20 mA, respectively. 𝑆𝐶𝐶𝑥 (%) = 𝑆𝐶𝐶 + 𝑆𝐶𝐶2 (4) where [TCE] in and [TCE] out are influent and effluent concentration in the gas stream. [CO] and [CO 2 ] are the concentration of carbon monoxide and carbon dioxide detected in the effluent gas and [TCE] conv is the concentration of TCE converted by the plasma. 3.1. TCE abatement with NTP Fig. 2 shows the TCE abatement and CO and CO 2 selectivity as a function of the energy density. As expected, with increasing energy density the abatement of TCE increases. Since higher energy density leads to higher energetic electrons which trigger the formation of radicals capable of decomposing TCE. For an energy density of 240 J/L the abatement and CO x selectivity reach a maximum at 80 % and 12 %, respectively. This low selectivity is related to the formation of unwanted and toxic by-products such as phosgene and dichloroacetylchloride [6]. Fig. 1. Schematic diagram of the experimental set-up. TCE concentration was controlled by changing feed gas (dry synthetic air) flow rate through TCE bubbling bottle by using mass flow controllers (MFC). A total air flow rate of 500 mL/min containing 500 ppm TCE was conveyed in all experiments. A FT-IR spectroscope (Bruker, Vertex 70) and a mass spectrometer (Hiden HPR-20) was used to identify and quantify by-products and TCE abatement. Spectra were taken after steady state condition and consisted of 10 averaged measurements. An UV ozone detector (Envitec, model 450) was used to monitor the formation of ozone. Cerium oxide (commercial catalyst) was calcinated for 4 h at 500 °C under 200 mL/min flow rate of dry synthetic air. For all tests, 0.5 g of CeO 2 powder was introduced in a cylindrical Pyrex glass reactor located in a temperature controlled vertical tubular oven. The temperature range was (100 - 500 °C) and (100 - 300 °C) for catalyst alone test and plasma-catalysis combined test, respectively. The oven was heated in a period of 60 min to the desired value. After obtaining thermal balance the measurements were performed. 3. Results and Discussion Abatement of TCE is investigated with only NTP, only heterogeneous catalyst and NTP-catalyst system (PPC). The examined parameters, TCE abatement (%), CO selectivity (𝑆𝐶𝐶 , %), CO 2 selectivity (𝑆𝐶𝐶2 , %) and CO x selectivity (𝑆𝐶𝐶𝑥 , %) are used to evaluate the process and are defined as follows: 𝑇𝑇𝑇 𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎 (%) = 𝑆𝐶𝐶 (%) = 𝑆𝐶𝐶2 (%) = 2 [𝐶𝐶] 2×[𝑇𝑇𝑇]𝑐𝑐𝑐𝑐 [𝐶𝐶2 ] 𝑇𝑇𝑇𝑖𝑖 −𝑇𝑇𝑇𝑜𝑜𝑜 × 100 2×[𝑇𝑇𝑇]𝑐𝑐𝑐𝑐 𝑇𝑇𝑇𝑖𝑖 × 100 × 100 (1) (2) Fig. 2. TCE abatement and CO and CO 2 selectivity as a function of the energy density. Table 1 shows the by-products of NTP treatment detected with FT-IR and MS. DCAC, phosgene, CO and CO 2 were observed with both techniques. Hence, the decomposition of TCE with NTP led to the formation of phosgene, DCAC and TCAA as incomplete oxidation products. These results are identical with Vandenbroucke et al. [6]. According to Kirkpatrick et al. [12], in TCE oxidation with NTP produces significant amount of DCAC by the following reaction: C 2 HCl 3 + ClO* → CHCl 2 COCl + Cl*. 3.2. TCE abatement with CeO 2 CeO 2 has been chosen as catalyst due to its unique properties, have higher oxygen storage/transport capacity [13] combined with the ability to shift easily between reduced and oxidized states (i.e., Ce3+ – Ce4+) which results in an increase in oxygen vacancies [14, 15]. It is also known that in association with other catalysts, ceria (3) O-3-6 can effectively reduce NO x emissions as well as convert harmful carbon monoxide to less harmful carbon dioxide. Fig. 3 shows the TCE abatement, CO, CO 2 and CO x selectivity as a function of the catalyst temperature with CeO 2 . The catalyst activity was evaluated for the temperature range of 100 - 500 °C. The plasma-catalytic abatement seems insensitive with the catalyst temperature. However, CO 2 selectivity increases more rapidly than CO selectivity, inevitably a large increase was observed for CO x selectivity (̴ 95%). Table 1. Detected by-products with NTP. By-product Structure FT-IR MS Unwanted Dichloroacetylchloride (DCAC) CHCl 2 COCl √ √ √ Trichloroacetaldehyde CCl 3 COH √ √ Phosgene COCl 2 √ √ √√ Hydrogen chloride HCl √ Chlorine Cl 2 Carbon monoxide CO √ √ Carbon dioxide CO 2 √ √ Ozone O3 √ √ √ √ Fig. 3 clearly shows that CeO 2 is not activate below 300 °C. Above this temperature the abatement increases and reaches maximum value of 51.6% at 500 °C. For a certain temperature range (300 – 400 °C), CO x selectivity remains constant ( ̴ 100%) while further increase of the temperature slightly decreases the selectivity. These results show that high temperature is essential to achieve moderate TCE abatement with high selectivity. Fig. 4. TCE abatement, CO, CO 2 and CO x selectivity as a function of the catalyst temperature for energy density 80 J/L. Fig. 5 shows the FT-IR analysis of plasma-catalysis combined system at energy density 40J/L with different catalyst temperature (100 - 200 °C). It is evident that with increasing catalyst temperature, the formation of chlorinated by-products (DCAC, phosgene) and O 3 are decreased . Simultaneously CO 2 selectivity increased proving that plasma-catalysis is an effective method for the complete oxidation of VOCs. Fig. 3. TCE abatement, CO, CO 2 and CO x selectivity as a function of the catalyst temperature. Fig. 5. FT-IR analysis of plasma-catalysis combined system at energy density 40J/L with different catalyst temperature (100 - 200 °C). 3.3. TCE abatement with combined system In order to reduce the energy cost of the process, we use low energy density plasma in combination with moderate catalyst temperature. Therefore, we operated the discharge at 40 J/L and 80 J/L and examined the process for catalyst temperatures between 100 - 300 °C. Fig. 4 shows the TCE abatement, CO, CO 2 and CO x selectivity as a function of catalyst temperature for energy density (80 J/L). 4. Conclusions The plasma-catalytic abatement of TCE showed a great improvement of the COx selectivity compared to the plasma alone system. By examining the effect of catalyst temperature, we found that low energy density plasma in combination with moderate catalyst temperature successfully abated dilute TCE in air streams. Future experiments will include a long term test (100 h) to test the stability of CeO 2 followed by a full characterization O-3-6 3 of the catalyst to examine if the catalyst morphology has changed and if catalyst poisoning has occurred. 5. Acknowledgements M. Mora acknowledges funding from Junta de Andalucia (FQM-6181), Ministry of Science and Innovation (MAT 2010-18778) and Fondos Feder. 6. References [1] P. Vineis, F. Forastiere, G. Hoek and M. Lipsett. Int. J. Cancer, 111, 5 (2004) [2] R. Atkinson. Atmosph. 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