Characterization of a direct dc-excited discharge in water by optical emission spectroscopy

被引:259
作者
Bruggeman, Peter [1 ,2 ]
Schram, Daan [3 ]
Gonzalez, Manuel A. [4 ]
Rego, Robby [5 ]
Kong, Michael G. [2 ]
Leys, Christophe [1 ]
机构
[1] Univ Ghent, Dept Appl Phys, B-9000 Ghent, Belgium
[2] Univ Loughborough, Dept Elect & Elect Engn, Loughborough LE11 3TU, Leics, England
[3] Tech Univ Eindhoven, Dept Appl Phys, NL-5600 MB Eindhoven, Netherlands
[4] Univ Valladolid, Dept Fis Aplicada, E-47011 Valladolid, Spain
[5] VITO Mat, Flemish Inst Technol Res, B-2400 Mol, Belgium
关键词
DIELECTRIC-BARRIER DISCHARGES; HYDROGEN STARK PROFILES; ATMOSPHERIC-PRESSURE; ELECTRON-DENSITY; ROTATIONAL TEMPERATURES; RADICAL FORMATION; BALMER LINES; ION DYNAMICS; PLASMAS; OH;
D O I
10.1088/0963-0252/18/2/025017
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
Dc-excited discharges generated in water at the tip of a tungsten wire which is located at the orifice of a quartz capillary are investigated by time-averaged optical emission spectroscopy. Two distinctive discharge modes are observed. For small conductivities of the liquid the discharge is a streamer-like discharge in the liquid itself (liquid mode). For conductivities above typically 45 mu S cm(-1) a large vapour bubble is formed and a streamer discharge in this vapour bubble is observed (bubble mode). Plasma temperatures and electron densities are investigated for both modes. The gas temperature is estimated from the rotational temperature of N(2) (C-B) and is 1600 +/- 200K for the bubble mode and 1900 +/- 200K for the liquid mode. The rotational temperature of OH (A-X) is up to 2 times larger and cannot be used as an estimate for the gas temperature. The rotational population distribution of OH(A), nu = 0 is also non-Boltzmann with a large overpopulation of high rotational states. This discrepancy in rotational temperatures is discussed in detail. Electron densities are obtained from the Stark broadening of the hydrogen Balmer beta line. The electron densities in the liquid mode are of the order of 10(21) m(-3). In the bubble mode electron densities are significantly smaller: (3-4) x 10(20) m(-3). These values are compared with the Stark broadening of the hydrogen alpha and gamma lines and with electron densities obtained from current density measurements. The chemical reactivities of the bubble and liquid modes are compared by means of the hydrogen peroxide production rate.
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页数:13
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