XIX-th ARS SEPARATORIA – Złoty Potok, Poland 2004 ISOTOPE EFFECTS FOR 34S/32S DURING DISSOLVING PROCESS OF SO2 IN POLAR SOLVENTS Agnieszka MIKOŁAJCZUK1), R. WIERZCHNICKI and Andrzej G. CHMIELEWSKI Instytut Chemii i Techniki Jądrowej, ul. Dorodna 16, 03-195 Warszawa, 1) [email protected] In this study sulfur fractionation factor between sulfur dioxide in gas phase and sulfur dioxide dissolved in three polar solvents has been investigated experimentally. Water, methanol and nitrobenzene were used in the experiment as solvents. Such measurements were carried out at the temperature range 20-70oC. The isotope composition was measured using mass spectrometry. The first investigation on sulfur isotope effects was experimentally performed in 1945 by Thode et al. [1]. The authors investigated the sulfur isotope effect in SO2(gas)-HSO3-(aq) system and found that the fractionation factor for the sulfur isotope pairs (34S/ 32S) and (36S/32S), was 1.019±0.02 and 1.043±0.02 at 25oC respectively. Such system is applied to the separation technology of sulfur isotopes till now [2]. Recently, sulfur isotope fractionation factors (34S/32S) were determined experimentally for the systems SO2 in the gas phase and dissolved in water [3] and methanol [4]. The isotope effects were investigated when these systems reached equilibrium states. and the solvent phases were saturated with sulfur dioxide. The influence of temperature on investigated sulfur isotopes separation between phases was studied as well. With increasing temperature, both the solubility of sulfur dioxide and the fractionation factor decrease, at 22oC α=1.00147, and at 70oC α=1.00086±0.000054 for SO2 saturated solutions. In the methanol isotope the fractionation factor is lower than in the water, and changes from α=1.00030 at 20oC to α =1.00041±0.00002 at 58oC. The solubility of sulfur dioxide in nitrobenzene is higher than in water and lower than in methanol. Sulfur dioxide dissolved in water reacts with the molecules of solvent. The precisely is not known which kind of structures is formed in methanol and nitrobenzene after SO2 dissolution. According to the force constant of the Lennard-Jones potential of gases and liquids the maximum solubility can be predicted. The force 222 XIX-th ARS SEPARATORIA – Złoty Potok, Poland 2004 constant of the Lennard-Jones potential of the liquids are 809.2K, 609.0K and 481.8K for methanol, nitrobenzene and water [6]. The solubility of gases in liquids depends on the force constant of the Lennard –Jones potential of the liquid. Methanol has the lowest force constant of the Lennard –Jones potential, than higher values have nitrobenzene and water, this is a reason that solubility of SO2 in methanol is the highest [6]. The nitrobenzene has the higher dipole moment than water and methanol. The values are 4.23D, 1.84D and 1.69D respectively. Sulfur dioxide has the dipole moment equal to 1.6D. Methanol is a polar solvent and creates hydrogen–bonds like water. Oxygen in -NO2 group creates hydrogen-bonding with donors of proton. Dielectric constants of dipolar liquids are large because dipolar molecules have a high free motion. In water the dielectric constant depends on a temperature, for example the dielectric constant at 25oC is equal to 78, at 100oC 55.33, for nitrobenzene 34.1 at 25oC and for methanol only 31.2 at 25oC. Water and methanol have the similar moment of dipole, both creates hydrogen-bonding, but solubility of SO2 in methanol is higher than in water; 35g of sulfur dioxide is dissolved at 20oC in methanol [4], 15.3 g in nitrobenzene and 10.64 g in water [5]. Figure 1 shows comparison sulfur isotope effects between sulfur dioxide in the gas and dissolved in water, methanol and nitrobenzene. 1.002 1.00175 1.0015 water [3] 1.00125 α 1.001 1.00075 1.0005 1.00025 methanol [4] 1 nitrobenzene 0.99975 0.9995 0.99925 10 20 30 40 50 60 70 80 temperature [oC] Fig. 1. Sulfur separation factor (α) between sulfur dioxide in the gas phase and liquid phase (water, methanol, nitrobenzene), solution saturated with sulfur dioxide, p=1013 hPa, precision of the measurement of δ34S is 0.052; 0.020; 0.013 respectively, for water, methanol and nitrobenzene. 223 XIX-th ARS SEPARATORIA – Złoty Potok, Poland 2004 In water and methanol the normal isotope effects were observed, while in nitrobenzene the reverse isotope effect was observed. The spectroscopic data to theoretical calculation are not available nowadays. The internal vibrational frequencies of SO2 molecule, when it is transferred from the gaseous into the “solvents” phase should be determined. Therefore, the fractionation factors were determined only experimentally in this work. When water was SO2 saturated, the isotope fractionation factor was equal to 1.00147 at 22oC, when the concentration SO2 in water was 0.292 mol/l (water partly saturated) the isotope fractionation factor was equal 1.00256 at 18oC [3]. In SO2 saturated water solution both, the solubility of sulfur dioxide and the fractionation factor decrease with increasing temperature, at 22oC α=1.00147, and at 70oC α=1.00086 ± 0.000052. In methanol the solubility of SO2 decrease with increasing temperature, however, the isotope fractionation factor changes from α = 1.00030 at 20oC to α=1.00041±0.00002 at 58oC. In this case, the changes of isotope fractionation factors were small and equal to about 0.15 ‰ [4]. In the case of nitrobenzene solution, the solubility of sulfur dioxide decrease when the temperature increase. In this case, the reverse isotope effect is observed, the heavier sulfur isotope is enriched in the gas phase in comparison with the solvent phase. The isotope fractionation factor changes from α=0.99961 at 20oC to α=0.99948± 0.000013 at 71oC. The changes of isotope effects are quite small, within the temperature range 20÷71oC, the changes are equal to about 0.18± 0.013‰. ACKNOWLEDGMENT This work was supported by a grant of Polish Committee for Scientific Research No. 4T09A 039 24. REFERENCES [1] [2] [3] [4] [5] [6] 224 H.G. Thode, R.L. Graham, J.A. Ziegler, Can. J. Research., 1945, B23, 40. W.K. Park, E.D. Michaels, Sep. Sci. Technol., 1993, 28, 477. A. Mikołajczuk, M. Derda, R. Wierzchnicki, A.G. Chmielewski, Nukleonika, 2002, 47, 69. A. Mikołajczuk, R. Wierzchnicki, A.G. Chmielewski, Czech. J. Phys., 2003, 53, 273. J. Zienkowicz, I. Senderacka, W. Wallmoden, Kalendarz chemiczny, PWT, Warszawa 1954. I.L. Leites, Sep. Purif. Technol., 1997, 12, 201.
© Copyright 2026 Paperzz