Abstract
The rate of solar coronal heating induced by the slow random motions of the dense photosphere is calculated in the framework of an essentially parameter-free model. This model assumes that these motions maintain the corona in a state of small-scale MHD turbulence. The associated dissipative effects then allow a large-scale stationary state to be established. The solution for the macroscopic coronal flow and the heating flux is first obtained assuming the effective (turbulent) dissipation coefficients to be known. In a second step these coefficients are calculated by the self-consistency argument that they should result from the level of turbulence associated with this very heating flux. For the sake of tractability the derivation is restricted to a two-dimensional situation where boundary flows are translationally symmetric. The resulting value of the heating rate and the predicted level of microturbulent velocity compare satisfactorily with the observational data.
| Original language | English |
|---|---|
| Pages (from-to) | 297-308 |
| Number of pages | 12 |
| Journal | Astrophysical Journal |
| Volume | 390 |
| Issue number | 1 |
| DOIs | |
| Publication status | Published - 1992 |
Keywords
- MHD
- Sun: corona
- Turbulence
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