Influence of Pressure and Oxygen Concentration on Nitrogen Isotope Separation in N2-O2 DC Discharge Nga Thi Anh Nguyen, Shinsuke Mori, Masaaki Suzuki Department of Chemical Engineering, Tokyo Institute of Technology 2-12-1 Ookayama, Meguro-ku, Tokyo 152-8552, Japan Abstract: Nitrogen isotope separation using plasma chemical reactions in N2-O2 electrical discharges system is performed in this study. The nitrogen isotope separation process has been investigated in the influence of oxygen concentration with a wide range of discharge pressure. The conversion of nitrogen increases with an increase in oxygen concentration. In atmospheric pressure, the lower oxygen concentration shows the higher nitrogen isotope separation factors in compensation for very small conversion of nitrogen. The highest nitrogen separation factor of 1.8 has been obtained at 0.03% of oxygen concentration in discharge of the N2-O2 mixture at atmospheric pressure. Keywords: nitrogen isotope, isotope separation, pressure, oxygen concentration 1. Introduction The enriched isotope of 15N has been used in various fields, such as agriculture, organic chemistry, life science, etc., as a non-radioactive tracer. Recently, greater attention has been given to the use of 15N in the nitride fuels of the fast breeder reactors (FBRs). Nitride fuels such as UN and PuN are known to have many desirable properties such as high melting point, high thermal conductivity and high breeding ratio. Since the (n, p) reaction of the abundant isotope 14N in natural nitrogen with neutron generates the radioactive 14C, the presence of isotope of 15N to avoid producing 14C elements in nitride fuels is a necessary replacement for environmental treatment. Therefore, enrichment of 15N is an important process for the implementation of nitride fuels. So far, many developments in nitrogen isotope separation processes have occurred. From the beginning, conventional methods have been conducted for the enrichment of the heavier nitrogen isotopes. These studies were the cryogenic distillation of NO with the separation factor of 1.027 or the ion exchange method in NH3-(NH4)2SO4 system with the separation factor of 1.021. However, these methods have some disadvantages in high energy consumption, multistage separation and environmental risk as well. For investigating alternative methods, in this study, we applied the plasma chemical reaction in N2-O2 electrical discharge for the nitrogen isotope separation process. In N2-O2 electrical discharges plasma system, vibrational excitation of the first few vibrational levels of a diatomic nitrogen molecule is operated by free electrons. With the collision of two vibrationally excited molecules, the excitation of a higher vibrational energy molecule having close vibrational level spacing is a faster process than that of the lower vibrational energy molecule having distant vibrational level spacing [1]. In addition, the isotopic effect reported by Belenov et al. [2] leads to the overpopulation of vibrational levels of a heavy component because of its closer spacing. 14 N 2 ( v ) + 14 N 15 N ( w ) → 14 N 2 (v − 1) + 14 N 15 N ( w + 1), w ≥ v (1) Therefore, the enrichment of 15N in the nitric oxide compound is achieved due to the difference in the rates of the chemical reactions of the molecules 14 14 N N and 14N15N (excited in vibrational levels ν ≥ 12) with O atoms [3]. N 2 ( v ≥ 12 ) + O → NO + N (2) The presence of oxygen and its concentration play important role in the reactions of (1) and (2). In 1995, Gordiets et al. [4] published a calculation about the effect of oxygen percentages on the nitrogen vibrational distribution at low pressure of N2-O2 glow discharge. The results demonstrated that the increase in oxygen percentage leads to the reduction of nitrogen vibrational distribution. In 2000, for another research of discharge at low pressure, there was a report about the effect of oxygen concentration on atomic nitrogen concentration of Kudrle et al. [5]. The authors observed that until a certain threshold, the concentration of atomic nitrogen rises rapidly with the amount of O2 admixture. If more O2 admixture is added, the concentration of nitrogen atoms decreases sharply. There was also in 2000, for the discharge at atmospheric pressure, Miralai et al. [6] mentioned about the oxygen concentration of 500ppm as a threshold to create atmospheric pressure glow discharge (APGD) in the nitrogen discharge. The total light emission from nitrogen APGD is mainly composed of the second positive system of N2. Then, adding the more oxygen gas exceeding the threshold could suppress this light emission. In this study, the influence of oxygen concentration of the discharge at low pressure and at atmospheric pressure on this nitrogen isotope separation process is addressed. 2. Experimental The experiments in this study were carried out according to the setup in the schematic shown in Figure 1. DC power supply was used to generate the glow discharge. The reaction zone was a U-shaped tube (7 mm I.D) made by Pyrex glass. Two stainless steel electrodes Ф 1 mm in the reaction zone had a 15 cm gap between them. The low energy electrons in the positive column are preferable for the vibrational excitation. Therefore, we utilize relatively long discharge tube. However, for the case discharge at atmospheric pressure, we reduced the discharge gap to 5 mm in order to be able to generate the discharge. The wall of the reaction U-tube was covered by the liquid nitrogen coolant. Flow conditions were set for all experiments. The discharge was generated between the gap of two electrodes to form the nitric oxide. DC Power Supply P1 P2 Reduction zone MS N2 O2 Copper Reaction zone Vacuum Pump Liquid N2 Liquid N2 Cold Trap Figure 1. Schematic of the experimental setup The natural nitrogen gas and oxygen gas were entered the reaction U-tube with a defined flow rate. The products containing nitric oxides were produced under the discharge. These products were supposed to condense on the cold wall of the U-tube reactor while the unreacted gases were pumped out with the flow. When the time for generating the discharge was finished, the reactor tube was closed and heated up to room temperature. At this time, the pressure (P1) inside reactor tube was recorded. The total amount of products was determined by this pressure (P1) of the products and the reactor volume. Since the products contained many kinds of species, which may affect the accuracy of the following analysis process, they were converted to nitrogen molecules again by the reduction reaction with copper threads [7]. The reduction zone was located next to the reaction zone and another U-shaped (5 mm I.D) quartz tube was used. The raw copper threads were placed inside this tube. The discharge products were transferred from the reaction U-tube to the reduction U-tube after measuring its pressure in reaction Utube at atmospheric temperature. Then, the reduction zone was closed and this reduction reaction was taken place at 800oC for five minutes. During the reduction time, the products containing nitric oxides reacted with the raw copper to release nitrogen gas forming copper oxide. After that, the pressure (P2) of the nitrogen gas in this reduction zone was recorded. The nitrogen separation factor was calculated based on the mass spectrometer 3. Results and Discussion In order to evaluate the efficiency of the enrichment of nitrogen isotope 15, the separation factor is defined by this formula: (15 N/ 14 N) products (15 N/ 14 N) reagents (3) Another parameter that is used to evaluate the amount of the collected nitrogen product in the process is the conversion of nitrogen. The formula for deriving this parameter is presented here: θN2 = 2 Mole of collected nitrogen gas .100% (4) Mole of nitrogen gas fed in which, the mole of collected nitrogen gas was calculated based on the pressure (P2) and the volume of the reduction zone at room temperature. 1.5 1 0.5 0 0 0.1 0.2 0.3 0.4 0.5 Oxygen Concentration (%) Figure 3. Effect of oxygen concentration on separation factor (atmospheric pressure) 0.2 Conversion of Nitrogen [x10 -4] (%) β= paper has reported. We hope we can make it in another discussion. Separation Factor measurements of the nitrogen gas in the reduction zone and the natural nitrogen gas. For further purification, after the reduction process, the mixed gases were passed by the cold trap 77 K before entering the mass spectrometer (MS). 0.15 0.1 0.05 0 0 0.1 0.2 0.3 0.4 0.5 Oxygen Concentration (%) Figure 2. Images of discharge at different oxygen concentration (atmospheric pressure) The images which display the discharge status at different oxygen flow rate were placed in Figure 2. The shape of the discharge at atmospheric pressure was affected significantly by the oxygen flow rate. At 0.5 sccm of oxygen flow rate, the discharge probably turns to arc discharge. The higher nitrogen separation factor was observed at the smaller oxygen concentration as in Figure 3. There is an agreement from this result with the previous study. The higher oxygen concentration reduces the efficiency of nitrogen isotope separation process. However, we still do not determine the threshold value of oxygen concentration as some Figure 4. Effect of oxygen concentration on conversion of nitrogen (atmospheric pressure) The conversion of nitrogen was calculated and presented in Figure 4. This results show the rather small value of conversion of nitrogen. The conversion of nitrogen increases reasonably with the increase in oxygen concentration. However, from Figure 3., the isotope selectivity of the chemical reaction reduces as the oxygen concentration rises. Figure 5. shows the images of discharge tube during and after the discharge generation at low pressure. Since there is almost no change of the shapes of discharge light with different oxygen concentration, thus, this figure presents the general discharge at low pressure. The blue color in the second image is the ozone condensation. Since the glass tube of N2-O2 Conversion of Nitrogen (%) discharge was cooled by liquid nitrogen, the ozone liquid was formed from the oxygen supply during the discharge. 0.14 0.12 0.1 0.08 0.06 0.04 0.02 0 0 During discharge After discharge Figure 5. Images of discharge tube (low pressure) Separation Factor The effect of oxygen concentration on the nitrogen separation factor in case of discharge at low pressure is observed in Figure 6. The separation factor has a maximum at value of 5%. This tendency is different from that of atmospheric discharge system. The discrepancy would be attributed to the rapid oxygen conversion into ozone liquid. As shown in Figure 5., oxygen is converted to ozone rapidly in the discharge tube at low pressure systems with liquid nitrogen coolant. Therefore, feed oxygen concentration can not reflect the practical oxygen concentration in the discharge tube. 10 20 Oxygen Concentration (%) Figure 7. Effect of oxygen concentration on conversion of nitrogen (low pressure) 4. Conclusion 1.6 The effect of oxygen concentration in the discharge at the low pressure and atmospheric pressure on the separation factor and the yield of nitrogen gas product have been investigated in this study. The higher oxygen concentration gives the lower nitrogen separation factor in the discharge at both low pressure and atmospheric pressure. The highest separation factor of 1.8 was observed at 0.03% of oxygen concentration in the discharge at atmospheric pressure. The conversion of the nitrogen was low because a very low oxygen concentration was used in the process. 1.5 References 1.4 1.3 1.2 1.1 1 0 5 10 15 20 Oxygen Concentration (%) Figure 6. Effect of oxygen concentration on separation factor (low pressure) The conversion of nitrogen at low pressure is shown in Figure 7. There is the same tendency of conversion of nitrogen of discharge at low pressure and at atmospheric pressure although the conversion in the atmospheric pressure system is much smaller than that of low pressure system. [1] C.E. Treanor, J.W. Rich, and R.G. Rehm, J. Chem. Phys., 48, 1798 (1968). [2] E.M. Belenov, E.P. Markin, A.N. Oraevskii and V.I. Romanenko, JETP Lett., 18, 116 (1973). [3] M. Capitelli, C.M. Ferreira, B.F. Gordiets, A.I. Osipov, ISBN 3-540-67416-0 Springer-Verlag Berlin Heidelberg New York, Plasma Kinetics in Atmospheric Gases, 246 (2000). [4] B.F. Gordiets, C.M. Ferreira, V.L. Guerra, J.M.A.H. Loureiro, J. Nahorny, D. Pagnon, M. Touzeau, and M. Vialle, IEEE Transactions on Plasma Science, 23 [4], 750 (1995). [5] V. Kudrle, A. Talsky, A. Kudlac, V. Krapek, J. Janca, Czechoslovak J. Phys., 50, Suppl. S3, 305 (2000). [6] S.F. Miralai, E. Monette, R. Bartnikas, G. Czeremuszkin, M. Latreche, and R. Wertheimer, Plasma and Polymers, 5 [2], 63 (2000). [7] T.J. Manuccia and M.D. Clark, Appl. Phys. Lett., 28, 372 (1976).
© Copyright 2025 Paperzz