GC-MS analysis of reaction products in nitrogen and methane gas mixture L. Polachova1,3, G. Horvath2,3, J. Watson4, N.J. Mason3, F. Krcma1, M. Zahoran2 and S. Matejcik2 1 Faculty of Chemistry, Brno University of Technology, Purkynova 119, 612 00, Brno, Czech Republic 2 Department of Experimental Physics, Comenius University, Mlynska dolina F-2, 842 48 Bratislava, Slovakia 3 Department of Physics and Astronomy, Open University, Walton Hall, Milton Keynes MK7 6AA, UK 4 Planetary and Space Sciences Research Institute, Open University, Walton Hall, Milton Keynes MK7 6AA, UK Abstract: Recent space missions have revolutionized our knowledge of planetary atmospheres in the solar system, most notably those of Mars and Titan. Simultaneously laboratory plasmas have been used to mimic the physical and chemical processes within such planetary atmospheres both to benchmark physico-chemical models and to interpret observations e.g. by providing plausible candidates for both spectral and mass spectrometric studies. In this paper we report the products formed in a gliding arc discharge fed by a 2 or 5% N2-CH4 gas mixture which mimics Titan’s atmosphere. Gas samples from the discharge exhaust were analyzed by GC-MS. Acetylene, hydrogen cyanide, and acetonitrile were found to be the major products. Minor detected products were: ethane, ethene, cyanogen, propene, propane, propyne, 1,2-propadiene, 1-butene3-yne, 1,3-butadiene, 1,3-butadiyne, 2-propenenitrile, 2-propanenitril, 2methylpropanenitrile, 2-methylpropanenitrile, benzene, and toluene. Whilst many of these compounds have been predicted and/or observed in Titan atmosphere the present plasma experiments provides evidence both of the chemical complexity of Titan and the mechanisms by which larger species grow prior to forming the dust that covers much of Titan’s surface Keywords: reaction nitrogen-methane gas mixture, gliding arc discharge, cold trap, Gas Chromatography-Mass Spectrometry. 1. Introduction Titan is the largest moon in Saturn’s lunar system and has been a subject of interest to astronomers and planetary scientists for a long time because the atmospheric conditions are thought to have resembled those conditions on the Earth several billion years ago [1]. Its atmospheric composition is principally nitrogen with 2–6 % of methane and some other gases that could be generated at low power discharges in the methane clouds [1]. The most important minor compounds detected by Cassini-Huygens space mission are nitriles (HCN, HC3N, HC5N, C2N2) believed to be formed as a result of dissociation of nitrogen and methane either by solar induced photolysis or by electron impact [2] and hydrocarbons (C2H2, C2H4, C2H6, C3H8, C3H4 [2]). In order to understand the physical and chemical processes leading to such observed phenomena additional laboratory simulations are required. Discharges have been shown to be good mimics of planetary atmospheres providing insights into both physical and chemical processes. DBD, glow, microwave, RF and corona discharges [3-11], have been all used in order to study electron-molecule and ion-molecule reactions in planetary atmospheres. In particular in recent years several of these discharges have been used to mimic Titan’s atmosphere and shown that various complex compounds can be formed, for example the higher hydrocarbons, nitriles or even amino acids. This paper presents the results of organic synthesis in a Titan like atmosphere operated in a Gliding Arc Discharge (GAD). We observe the production of C6 to C9 hydrocarbons from methane in the discharge. To understand the molecular kinetics during the discharge, the energy distribution as well as knowledge of plasma composition is necessary. In this paper we provide our results of a qualitative and quantitative GC-MS analysis of gliding arc discharges fed by a CH4 – N2 gas mixture. 2. Experiment The apparatus used in our experiments is shown schematically in Figure 1. The flow rates through the reactor for both CH4 and N2 were regulated using MKS mass flow controllers. The measurements were carried out in a flow regime over a range from 100 and 200 ml min-1 at atmospheric pressure and laboratory temperature. The discharge electrode system had the standard configuration of a classical gliding arc. A pair of stainless steel holders was positioned in parallel to the iron electrodes, but in this case the plasma was not gliding due to the low flow rate. Astable abnormal glow plasma occurred between the electrodes at their shortest distance of 2 mm, and a plasma channel with diameter of 1 mm was formed. The electrical parameters were measured by a Tektronix oscilloscope using high voltage probe and Rogowsky current probe. The reactor chamber had a volume of 0.3 L. The discharge was powered by a DC HV source. The discharge was ignited at 5500 V, then voltage drop reached a value at about 400 V but with increasing current (between 15 and 40 mA) the voltage was found to slightly decrease from 400 to 350 V. The present experiments were performed for different N2:CH4 ratios in range from 2 % and 5 % methane in nitrogen. Gaseous samples of the products formed in the discharge were taken out for GC-MS analysis through a gas outlet into a cold trap. The cold trap was subsequently heated and the resultant gas sample for GC-MS analysis was taken using a lock syringe before being immediately analyzed using Gas Chromatography and Mass spectrometry. GCMS analysis was carried out using an Agilent Technologies 6890 gas chromatograph coupled to a 5973 mass spectrometer. Separation was performed on a J&W GS-Q PLOT column (30 m in length, 0.32 mm internal diameter). Helium with a column flow rate of 2 sccm was used as the carrier gas. Injection was at a 5:1 split and injector temperature was 220 °C. The GC oven temperature was held for 2 min at 35 °C and then programmed at 10 °C min−1 upto 220 °C with the final temperature held for 5 min. The MS was operated in electron impact (70 eV) mode and scanned between 12-120 amu at approximately 11 scans/sec. Figure 1. Experimental set up: 1- storage bottle of nitrogen, 2storage bottle of methane, 3- MKS mass flow controllers, 4- DC power supply, 5- oscilloscope, 6- electrode system, 7- reactor body, 8- IR gas cell, 9- FTIR spectrometer, 10- cold trap for GC-MS, 11- exhaust. 3. Results and discussion The example of results from GC-MS analysis are shown in Figure 2. Various compounds were detected, for example the hydrocarbons: ethene, acetylene, ethane, propene, propane, propyne, 1,2propadiene, 1-butene-3-yne, 1,3-butadiene and 1,3butadiyne. The following nitriles were also identified: hydrogencyanide, acetonitrile, cyanogen, 2-propenenitrile, 2-propanenitrile, 2-methylpropenenitrile and 2-methylpropanenitrile. Benzene and toluene were detected as the aromatic compounds. The concentration of acetylene, hydrogen cyanide, and acetonitrile were higher than expected but it should be mentioned that only products having quantitative (peak area) higher than 106 have been considered in the analysis. Many of these compounds have been detected or are predicted to be in Titan’s atmosphere. Figure 3. Results of quantitative analysis for major products formed in the discharge at different concentration of CH4-N2 gas mixture. Figure 2. Sample GC-MS spectrum of analysed products formed in a gas mixture CH4:N2 = 2:98 at flow rate of 200 ml min-1. Figure 3 shows the quantitative analysis of some hydrocarbons formed under different experimental conditions. The quantitative unit is represented by a peak area. As is shown in Figure 3, the concentration depends on the initial methane content. Figure 3 shows the concentration of major products (ethene, acetylene, ethane, cyanogen, propene, hydrogen cyanide, acetonitrile, propenenitrile, propanenitrile). Since these experiments have been carried out for different CH4-N2 mixture ratios and the same gas flow rates, the evolution of different product concentrations was found to depend strongly on the initial gas ratios. The dependence of product concentrations is strongly dependent on the different CH4-N2 gas mixtures. An increase in the initial CH4 content from 2 to 5% caused a major increase in all the product yields, however, there was a more significant effect on some hydrocarbon-like products than others: the yield of all N-containing products increased rapidly but was less dramatic in the hydrocarbons and hydrogen cyanide yields. Figure 4 shows the quantitative unit (peak area) of the major products formed at various flow rates and the same CH4 content. Increasing the flow rate of the gas mixture CH4-N2 content from 100 to 200 sccm causes a decrease in the total product yield. Furthermore, as it was expected, lowering the flow rate of the gas mixture produced higher yields of products. The highest yield for all products was reached for 2% of CH4 at the lowest flow rate. Figure 4. Results of quantitative analysis for major products formed in the discharge with different experimental flow rates and the same methane concentration. Figure 5 shows the same situation as above but at higher methane concentration. Comparing figures 4 and 5, mixtures prepared under identical conditions but with different methane concentration in the gas mixture showed that lowering the flow rate of the gas mixture produced higher concentrations of the products. The highest yield of all products was reached for 5 % of CH4 at the lowest flow rate. Figure 5. Results of quantitative analysis for major products formed in the discharge at different experimental flow rates abut with the same methane concentration. 4. Conclusion In this contribution we present the results of a GCMS study of stable gaseous products formed in the gliding arc discharge fed by different atmospheric pressure mixtures of N2:CH4 (2 and 5 % of CH4) operated in a flowing regime with a discharge current of 30 mA at room temperature and atmospheric pressure. Ex situ GC-MS analysis of the gaseous products showed that HCN, C2H2, CH3CN are the major products in our CH4/N2 non-thermal plasma. The yields of these compounds are as follows: HCN >C2H2> CH3CN. Minor detected products were: ethane, ethene, cyanogen, propene, propane, propyne, 1,2-propadiene, 1-butene-3-yne, 1,3-butadiene, 1,3-butadiyne, acetonitrile 2propenenitrile and 2-propanenitrile, 2methylpropanenitrile, 2-methylpropanenitrile, benzene and toluene. Such experiments can provide information that could aid our understanding of processes in Titan’s atmosphere. Acknowledgements. This work has been supported by the Grant UK/140/2010, Slovak Research and Development Agency VEGA 1/0051/08, APVV 0365-07, ESF COST Actions CM0601, CM0805 and EUROPLANET TNA2. Research plan of Czech Ministry of Education No. MSM 0021630501 and Czech Science Foundation project No. 104/09/H080 supported this research, too. References [1] Aplin K. L., Surveys in Geophysics, vol. 27, pp 63-108, 2006. [2] Vinatier S. et al., Icarus 188, pp 120-138, 2007. [3] Bernard J M, Quirico E, Brissaud O, Montagnac G, Reynard B, McMillan P, Coll P, Nguyen M J, Raulin F and Schmitt B, Icarus 185 301, 2006. [4] Pintassilgo C. D., Loureiro J., Cernogora G. and Touzeau M., Plasma Sources Sci. Technol. 8 463, 1999. [5] Szopa C., Cernogora G., Boufendi L., Correia J. and Coll P., Planetary and Space Science 54 394, 2006. [6] Imanaka H., Khare B. N., Elsila J. E., Bakes E. L. O., McKay C. P., Cruikshank D. P., Sugita S., Matsui T. and Zare R. N., Icarus 168 344, 2004. 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