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Astron. Astrophys. 325, 709-713 (1997) 4. ConclusionsI have presented new calculations for the generation of sub- and
supersonic inflows and outflows in the chromosphere of
1. In case of stochastic shock waves the mechanical energy and momentum input to the atmosphere occurs episodically and is overwhelmingly controlled by strong shocks generated by shock merging. These shocks are thus responsible for generating stochastic chromospheric velocity fields. 2. In case of stochastic shocks, a relatively broad range of
chromospheric velocities is encountered, which increases with
decreasing mass column density. In the middle and outer chromosphere,
the characteristic velocity range encompasses 3. The difference between the chromospheric velocity distributions for the two inserted spectra appear to be insignificant. A much narrower velocity distribution however is found in case of the monochromatic wave model considered. 4. The range of velocities found in the stochastic wave
computations appear to be consistent with the velocity intervals
revealed by the Fe II emission line components observed by
HST-GHRS, which are considered an important diagnostic tool for
chromospheric dynamics of 5. Regarding the Mach numbers of the flow, it is found that supersonic inflows and outflows are easily produced by the stochastic wave models, contrary to the monochromatic wave model calculated. This result is in agreement with earlier results given by Cuntz (1992a, b). 6. In case that noninstantaneous ionization of hydrogen is
considered, some of the results are expected to change, notably the
This work is part of ongoing efforts to understand outer
atmospheric heating in stars of different spectral type and
evolutionary status. In case of ![]() ![]() ![]() ![]() © European Southern Observatory (ESO) 1997 Online publication: April 28, 1998 ![]() |