22nd International Symposium on Plasma Chemistry July 5-10, 2015; Antwerp, Belgium Conversion of CO 2 and H 2 O by microwave plasma discharge coupled with a catalytic reactor G. Chen1,2, V. Georgieva1, T. Godfroid3, T. Silva2, N. Britun2, R. Snyders2,3 and M.-P. Delplancke-Ogletree1 1 4MAT, Université libre de Bruxelles, 50 av. F.D. Roosevelt, 1050 Brussels, Belgium 2 ChIPS, Université de Mons, 23 Place du Parc, 7000 Mons, Belgium ³ Materia Nova Research Center, av. N. Copernic 1, 7000 Mons, Belgium Abstract: In this work, the conversion of CO 2 and H 2 O vapor mixture in a microwave plasma system in presence of NiO/TiO 2 catalyst is investigated. The results show that the CO 2 conversion depends on the crystal phase of the catalyst support. I t increases when NiO/TiO 2 (anatase) and NiO/TiO 2 (anatase/rutile mixture) are used, while NiO/TiO 2 (rutile) lead to lower CO 2 conversion efficiency in comparison with the plasma only assisted dissociation. Keywords: CO 2 /H 2 O conversion, plasma-catalysis, NiO/TiO 2 catalyst 1. Motivation Decrease of natural reserves of fossil fuels and the greenhouse effect from CO 2 emissions generated by anthropomorphic activity incites searching for new sources of fuels. The most generally useful method is the conversion of electrical energy produced by renewable or nuclear source into a chemical fuel. One of the promising solution is using the electrical energy for plasma processing CO 2 to convert it into synthetic fuels [1]. Recently, the combination of heterogeneous catalysis and plasma activation, known as plasma-catalysis, has attracted increasing interest. The dissociation of CO 2 was extensively studied in the recent years [2-7]. However, in order to produce synthetic gas (CO/H 2 ) H 2 has to be added. The production of hydrogen is expensive as it takes a great deal of energy to extract it from water. Therefore, it is of practical interest to investigate the simultaneous dissociation of CO 2 and H 2 O. Up to now, few studies have investigated the steam reforming of CO 2 by plasma [8, 9]. In this paper, the conversion of CO 2 and H 2 O mixtures in presence of titanium oxide supported NiO in a surfacewave sustained microwave discharge is, to our knowledge, investigated for the first time. The aim is to evaluate the conversion efficiency dependence on the catalyst properties. containing the catalyst is connected to the end of the quartz tube. The pressure in the discharge tube is set to 1330 Pa for all experiments. The whole system is surrounded by a grounded aluminum grid to prevent any leak of microwave radiation into the outer space. Pulse duration is set to 300 µs, and the off period is set to 300 µs. A more detailed description of the microwave set-up can be found in [9]. 2. Experiments 2.1. Experimental system Fig. 1 shows a schematic diagram of the experimental setup. The discharge is sustained by microwave radiation (915MHz) in a quartz tube, 14 mm in inner diameter and 24 cm long surrounded by a Plexiglas tube of 28 mm inner diameter. The discharge tube is cooled by silicon oil flowing between the inner and the outer tubes. CO 2 and H 2 O gas mixture is injected from the top of the system. The water vapor is generated in a vaporization system built by Omicron technologies. A reactor Fig. 1. Schematic representation of surface-wave microwave set-up. O-12-5 2.2. Catalyst preparation The NiO supported on TiO 2 catalysts were prepared by combination of impregnation and plasma treatment methods. The precursor was Ni(NO 3 ) 2 • 6H 2 O (Merck). TiO 2 nanocrystalline powder (Sigma-Aldrich) in two polymorphs (anatase, rutile, and a mixture of rutile and anatase) were used as a catalyst support. The mixture consists of 86.5% anatase and 13.5% rutile. TiO 2 support 1 was impregnated with the aqueous solution of Ni(NO 3 ) 2 • 6H 2 O for 24 hours and dried at 100 ℃ for 12 hours, followed by CO 2 plasma treatment of 30 minutes at a plasma power of 2000 W to form NiO/TiO 2 catalysts. The three catalysts were denoted NiO/TiO 2 (anatase), NiO/TiO 2 (rutile) and NiO/TiO 2 (mixture), respectively. 2.3 Product analyses The composition of the post-discharge is analyzed by a gas chromatograph (GC) (Bruker) equipped with a carbon molecular sieve column and a Molecular sieve 5A column in series and connected to a thermal conductivity detector, which allows to determine the concentration of H 2 , O 2 , CO and CO 2 . The conversion of CO 2 is calculated by comparing the peak area of CO 2 obtained by the GC before and after reaction. The conversion efficiency of CO 2 and the yield of CO (and H 2 ) are calculated based on the following ratios: CO2 Conversion (%) = Yield of CO(H2 ) = moles of CO2 converted moles of CO2 in feed × 100% moles of CO(H2 ) produced × 100% moles of CO2 (H2 O) in feed 3. Results and discussion The following operating parameters are used in the present study: CO 2 /H 2 O (90%:10%) gas mixture is supplied at flow rate of 2 slm, and input power of 2000 W, which corresponds to a specific energy input per molecule of 6.95 eV/molecule. Comparisons of CO 2 conversion using the surface-wave microwave with and without catalysts as well as the effect of the titanium oxide supported NiO catalysts are shown in Fig. 2. 5 g of the catalysts (10 wt.% NiO/TiO 2 ) were used for each experiment, corresponding to a space velocity of 24,000 ml/(h.g). As can be noted from Fig. 2, the CO 2 conversion was significantly enhanced when NiO/TiO 2 (mixture) is used. The CO 2 conversion increases from 43% to 66%, comparing with the plasma only experiment. With NiO/TiO 2 (anatase), the CO 2 conversion initially increases and reaches stable values around 60% with the catalyst activation. The results show that coupling plasma with catalysts allows modifying the conversion efficiency of CO 2 . This can result from different phenomena. The CO 2 can be decomposed on the catalyst surface which explains the improvement observed. It is also possible that water decomposes on the catalyst. The H 2 formed by this reaction can react with the CO 2 to produce CO and water through the reverse water gas shift reaction (WGSR). On the other hand, NiO/TiO 2 (rutile) catalyst did not affect CO 2 conversion efficiency. Fig. 3 shows the X-ray powder diffraction patterns of NiO supported on TiO 2 catalysts in different crystal phases. The XRD patterns confirmed the crystal structure of these three catalysts. The crystallite sizes of catalysts were estimated from the XRD patterns according to the 2 Scherrer’s formula, and the data are listed in Table 1. The crystallite size of NiO/TiO 2 (rutile) is 51 nm. However, a Fig. 2. Comparison of CO 2 conversion efficiencies in pure plasma and the combined effects of plasma and catalyst in CO 2 /H 2 O mixture. small crystallite size was noticed for the other two catalysts. Very weak diffraction peaks observed in the diffraction pattern in the diffraction pattern of NiO/TiO 2 (anatase) catalyst at 2θ = 43.5, correspond well with the (200) crystal planes of face-centered cubic NiO. In addition, no NiO diffraction peaks could be observed from the XRD measurements of NiO/TiO 2 (mixture) catalyst, suggesting that the nickel oxide is either highly dispersed on the support or the crystallite size is below the XRD resolution limit. Fig. 3. XRD patterns of TiO 2 supported NiO catalysts: b) NiO/TiO 2 (rutile); and a) NiO/TiO 2 (anatase; c) NiO/TiO 2 (mixture). Table 1 also compares the measured BET surface area, porosity and total pore area. NiO/TiO 2 (rutile) had the lowest BET surface area (m2/g), almost one quarter as much as that of NiO/TiO 2 (mixture) and one fifth as much as that of NiO/TiO 2 (anatase). The porosities of the three O-12-5 catalysts were similar. However, higher total pore areas were observed for NiO/TiO 2 (anatase) and NiO/TiO 2 (mixture) catalysts. Table 1. Properties of TiO 2 supported NiO catalysts. catalyst Property Crystallite size (nm) Porosity (%) Total pore Area (m2/g) BET surface area (m2/g) NiO/TiO 2 (Anatase) NiO/TiO 2 (Rutile) NiO/TiO 2 (mixture) 17 51 20 44.1 51.5 43 9.3 58.4 58.6 58 12 49 Fig. 4a-c shows the scanning electron microscope images of TiO 2 supported NiO catalysts. As shown in Fig. 4, smaller particle and uniform size distribution can be observed for the NiO/TiO 2 (anatase) and NiO/TiO 2 (mixture) catalysts. This observation is in agreement with the XRD results. However, comparing them, the NiO/TiO 2 (rutile) catalysts exhibited larger particle, and particles agglomerated to form block-like crystal. use in the microwave reactor by state-of-the art tools such as X-ray photoelectron spectroscopy (XPS), Raman spectroscopy, Time of Flight Secondary Ion Mass Spectrometry (ToF-SIMS) and CO 2 Temperature Program Desorption (CO 2 -TPD). The corresponding research is ongoing and further studies regarding this subject will be reported in future. 4. Acknowledgments This research is carried out in the framework of the network on Physical Chemistry of Plasma Surface Interactions - Interuniversity Attraction Poles phase VII project (http://psi-iap7.ulb.ac.be/), supported by BELSPO. NB is a post-doctoral researcher of the Fonds National de la Recherche Scientifique (FNRS), Belgium. 5. References [1] A.P.H. Goede, W.A. Bongers, M.F. Graswinckel, M.C.M van de Sanden, M. Leins, J. Kopecki, A. Schulz and M. Walker. Eur. Phys. J. Web of Conferences, 79, 01005 (2014) [2] S.L. Brock, M. Marquez, S.L. Suib, Y. Hayashi and H. Matsumoto. J. Catal., 180, 225-233 (1998) [3] J.Y. Wang, G.G. Xia, A. Huang, S.L. Suib, Y. Hayashi and H. Matsumoto. J. Catal., 185, 152-159 (1999) [4] R. Li, Y. Yamaguchi, S. Yin, Q. Yang and T. Sato. Solid State Ionics, 172, 235-238 (2004) [5] R. Li, Q. Tang, S. Yin and T. Sato. Fuel Process Technol., 87, 617-622 (2006) [6] G., Horvath, J.D. Skalny and N.J. Mason. J. Phys. D: Appl. Phys., 41, 225207 (2008) [7] L.F. Spencer and A.D. Gallimore. Plasma Sources Sci. Technol., 22, 015019 (2013) [8] S. Mahammadunnisa, L. Reddy, D. Ray, C. Subrahmanyam and J.C. Whitehead. Int. J. Greenh. Gas Con., 16, 361-363 (2013) [9] G. Chen, T. Silva, V. Georgieva, T. Godfroid, N. Britun, R. Snyders and M.-P. DelplanckeOgletree. Int. J. Hydrogen Energy, 40, 3789-3796 (2015) Fig. 4. SEM micrographs of TiO 2 supported NiO catalysts: a) NiO/TiO 2 (anatase); b) NiO/TiO 2 (rutile); and c) NiO/TiO 2 (mixture). The higher activity observed in the plasma treatment using NiO on TiO 2 (anatase) and (mixture) catalysts may be linked to the formation of well-dispersed NiO particles, large surface area and small crystallite size. The fundamental mechanisms of reactions are still unknown and, therefore, further investigations are necessary. To get a better understanding of the relationship between the plasma-catalyst interactions and synergistic effect of plasma-catalysis from both a chemical and physical perspective, characterization of the different catalysts before and after their utilization must be done. Particularly, the chemical composition and morphology of the catalysts will be characterized before and after their O-12-5 3
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