22nd International Symposium on Plasma Chemistry July 5-10, 2015; Antwerp, Belgium Spectroscopic studies of sonoluminescence of the N 2 /Ar/H 2 O system to probe the non-equilibrium plasma in cavitation bubbles T. Ouerhani, R. Pflieger and S.I. Nikitenko Institut de Chimie Séparative de Marcoule, UMR5257, UM2-CEA-CNRS, Centre de Marcoule, Bat. 426, P.O. Box 17171, FR-30207 Bagnols-sur-Cèze cedex, France Abstract: Spectroscopy of sonoluminescence and follow up of the sonochemical products are two ways of studying the SC plasma. Though, their links are poorly understood. This work focuses on the N 2 /Ar/H 2 O system using both approaches at various ultrasonic frequencies. Besides, the temperature characteristics of the plasma (vibrational and rotational temperatures of NH) are estimated using Specair software. Keywords: plasma, spectroscopy, sonoluminescence, sonochemistry Sonochemistry, or in other words the chemical effects of ultrasound, originates from acoustic cavitation: nucleation, growth and implosive collapse of gas bubbles in liquids submitted to an ultrasonic field. The implosion occurs on the microsecond time scale and induces extreme local conditions of temperature and pressure. A non-equilibrium plasma is formed that emits light, the socalled sonoluminescence (SL). Spectroscopic studies of SL are a major tool to investigate the plasma conditions (temperatures and pressure [1, 2]) created by acoustic cavitation in liquids. The spectra of SL typically show an intense continuum ranging from the UV to the NIR, usually attributed to bremsstrahlung, radical recombination and water molecule emission, on top of which emission peaks from excited species are present, like OH (A-X) and OH (C-A) in water sparged with Ar. The shape of these molecular emissions reflects the vibrational and rotational temperatures of the considered species. In the present work the SL spectra of water sparged with Ar/N 2 gas mixtures are systematically studied in a large range of ultrasonic frequencies (20, 204, 362, 613 and 1057 kHz) using the multifrequency sonoreactor described recently [3]. At 20 kHz, the sole molecular emission is that of OH (A-X). On the contrary, at high frequency a second emission is present, namely that of NH(A-X) system (Fig. 1). Comparison of experimental NH(A-X) spectra with emission spectra obtained using Specair software [4] allow to estimate NH(A-X) vibrational and rotational temperatures, and therefore to assess the plasma conditions. Besides, the rate of formation of sonolysis products was followed during the sonolysis of water sparged with various Ar/N 2 mixtures: W H2 by mass spectrometry, W H2O2 and W NO2- by absorption spectroscopy and W NO3by ion chromatography method. A comparison of NH emission in MBSL and sum of formation rates of NO 2 and NO 3 - as a function of N2 content in Ar is shown in Fig. 2. Based on the comparison of the SL and the P-I-2-52 sonochemical results, the mechanisms of the reactions occurring in the cavitation bubbles are proposed (Fig. 3). Fig. 1. SL spectrum of water sparged with Ar/ 14% N 2 at 359 kHz, P ac = 50 W, T = 11 °C. Fig. 2. Peak height of NH emission in SL and sum of formation rates of NO 2 - and NO 3 - as a function of N 2 content in Ar at 359 kHz, P ac = 50 W and T = 11 °C. 1 Fig. 3. Mechanism of formation of NO 2 - and NO 3 -. References [1] E.B. Flint and K.S. Suslick. Science, 253, 1397-1399 (1991) [2] M.V. Kazachek and T.V. Gordeychuk. Techn. Phys. Lett., 35, 193-196(2009) [3] N.M. Navarro, R. Pflieger and S.I. Nikitenko. Ultrason. Sonochem., 21, 1026-1029 (2014) [4] C.O. Laux, T.G. Spence, C.H. Kruger and R.N. Zare. Plasma Sources Sci. Technol., 12, 125-138 (2003) 2 P-I-2-52
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