Abstract
The statistical equilibrium equations for the continuum and first 10 levels of a hydrogen atom show that the radiation of a bright prominence (the brightness of the Hα line has attained 56 mÅ of the disc centre spectrum) is completely due to scattering of the Sun radiation. The basic unknowns are separated with certainty: electron concentration (n e = 3.0 × 1010 cm−3), effective thickness (l = 4.2 × 108 cm) and electron temperature (T e = 5000 K).
Radiation of a very bright prominence (A λ(Hα) = 213 mÅ; T e = 7300 K; n e = 5.0 × 1011 cm−3; l = 1.3 × 107 cm) is on account of electron impacts (40%) and the Sun radiation scattering (60%).
The parameters are shown to depend greatly on the prominence optical thickness in the lines of the first subordinate series of a hydrogen atom. In the course of determination all the parameters and 100 interconnected integral equations of the radiation diffusion have been thickness-averaged; the population of levels has been calculated by observations using the self-absorption factors.
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Chultem, T., Yakovkin, N.A. Stationary equations of hydrogen excitation and ionization in prominences. Sol Phys 34, 133–150 (1974). https://doi.org/10.1007/BF00149605
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DOI: https://doi.org/10.1007/BF00149605