Temperature measurement in thermal plasmas by Rayleigh scattering

The range of temperatures over which Rayleigh scattering is a useful diagnostic of temperature in a noble gas thermal plasma at atmospheric pressure is examined. The various scattering processes that can occur a light passes through such a plasma are outlined. It is shown that while Rayleigh scattering by ground-state atoms is the dominant process at low temperatures, Thomson scattering becomes important at temperatures at which significant ionization occurs. Resonance scattering is also a significant source of scattered radiation when the laser wavelength is approximately equal to the wavelength of a transition of a species present in the plasma. Radial profiles of the polarized and depolarized radiation scattered from argon and helium arcs have been measured and analysed to confirm the relative importance of the respective scattering mechanisms. The occurrence of Thomson scattering is found to set a fundamental upper-temperature limit to the applicability of Rayleigh-scattering techniques to temperature measurement. For a laser wavelength of 514.532 nm and a detection system bandwidth of less than 0.1 nm, Thomson scattering becomes significant at approximately 9000 K in argon and 11000 K in helium. Above these values, the derivation of plasma properties from scattering measurements requires that all scattering mechanisms be taken into account. The temperature of the argon arc is calculated to exemplify this.

[1]  Carl M. Penney,et al.  Light Scattering in Terms of Oscillator Strengths and Refractive Indices , 1969 .

[2]  R. Kearney,et al.  Rayleigh scattering from an argon plasma jet at atmospheric pressure , 1990 .

[3]  K. Steuer,et al.  Rayleigh Scattering from Excited Atoms in Plasmas , 1976 .

[4]  G. Haddad,et al.  Temperature determinations in a free-burning arc. I. Experimental techniques and results in argon , 1984 .

[5]  D. Posener.  The Shape of Spectral Lines : Tables of the Voigt Profile (a/pi)?8-8e-y2dy/{a2+(nu-y)2} , 1959 .

[6]  J. Keck,et al.  MONTE CARLO TRAJECTORY CALCULATIONS OF ATOMIC EXCITATION AND IONIZATION BY THERMAL ELECTRONS. , 1969 .

[7]  R. Hanson,et al.  Simultaneous planar measurements of velocity and pressure fields in gas flows using laser-induced fluorescence. , 1988, Applied optics.

[8]  Noel A. Clark,et al.  Inelastic light scattering from density fluctuations in dilute gases. The kinetic-hydrodynamic transition in a monatomic gas , 1975 .

[9]  D. Crosley,et al.  Polarization of laser-induced fluorescence in OH in an atmospheric pressure flame. , 1984, Applied optics.

[10]  L. Poladian,et al.  Departures from equilibrium in a free-burning argon arc , 1988 .

[11]  Leendert Vriens,et al.  Cross-section and rate formulas for electron-impact ionization, excitation, deexcitation, and total depopulation of excited atoms , 1980 .

[12]  Leendert Vriens,et al.  Light scattering from Ne, Ar, and Xe arcs , 1974 .

[13]  G. Haddad,et al.  Rayleigh scattering measurements in a free-burning argon arc , 1988 .

[14]  A. D. May,et al.  Rayleigh-Brillouin spectrum of compressed He, Ne, and Ar. I. Scaling , 1980 .

[15]  V. Helbig,et al.  Non-LTE diagnostic of an argon arc plasma , 1984 .

[16]  N. Konjević,et al.  Experimental Stark Widths and Shifts for Non-Hydrogenic Spectral Lines of Ionized Atoms (A Critical Review and Tabulation of Selected Data), , 1976 .

[17]  D. Evans,et al.  Laser light scattering in laboratory plasmas , 1969 .

[18]  R. Décoste,et al.  Density and Temperature Profile Measurement on a Transferred Arc Plasma Using CW Laser Scattering , 1987, IEEE Transactions on Plasma Science.