The Role of Helium in the Outer Solar Atmosphere
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Citation V. H. Hansteen et al 1997 ApJ 482 498DOI 10.1086/304111
V. H. Hansteen
AFFILIATIONS
Institute of Theoretical Astrophysics, University of Oslo, P.O. Box 1029, Blindern, N-0315 Oslo; and High Altitude Observatory, National Center for Atmospheric Research, 3450 Mitchell Lane, P.O. Box 3000, (The National Center for Atmospheric Research is sponsored by the National Science Foundation.) Boulder, CO 80307
E. Leer
AFFILIATIONS
Institute of Theoretical Astrophysics, University of Oslo, P.O. Box 1029, Blindern, N-0315 Oslo; and High Altitude Observatory, National Center for Atmospheric Research, 3450 Mitchell Lane, P.O. Box 3000, (The National Center for Atmospheric Research is sponsored by the National Science Foundation.) Boulder, CO 80307
T. E. Holzer
AFFILIATIONS
High Altitude Observatory, National Center for Atmospheric Research, 3450 Mitchell Lane, P.O. Box 3000, Boulder, CO 80307
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Dates
- Received 1996 May 28
- Accepted 1997 January 13
Abstract
We construct models of the outer solar atmosphere comprising the region from the mid-chromosphere and into the solar wind in order to study the force and energy balance in models with a significant helium abundance. The corona is created by dissipation of an energy flux from the Sun. The energy flux is lost as radiation from the top of the chromosphere and as gravitational and kinetic solar wind energy flux. We find that in models with significant ion heating of the extended corona most of the energy flux is lost in the solar wind. The ion temperatures are higher than the electron temperature in these models, and the α-particle temperature is much higher than the proton temperature, so there is energy transfer from the α-particle fluid to the protons and electrons, but this energy exchange between the different species is relatively small. To a fairly good approximation we can say that the energy flux deposited in the protons and α-particles is lost as kinetic and gravitational energy flux in the proton and α-particle flow. How this energy flux is divided between gravitational and kinetic energy flux (i.e., how large the particle fluxes and flow speeds are) depends upon details of the heating process. We also find that mixing processes in the chromosphere play an important role in determining the coronal helium abundance and the relative solar wind proton and α-particle fluxes. Roughly speaking, we find that the relative α-particle and proton fluxes are set by the degree of chromospheric mixing, while the speeds are set by the details of the coronal heating process.
