http://arxiv.org/abs/1903.09993
The equilibrium of current-carrying magnetic fields (e.g. flux tubes) embedded in a large-scale background field is developed and discussed in the astrophysical context. Embedded non-force-free current-carrying fields require a minimum surrounding atmosphere, which by direct pressure balance has a gas pressure everywhere proportional to the background magnetic pressure. Formally, the MHD equations, with flows and gravity as part of a wide class of physical processes, separate into independent local and global relations representing an equilibrium solution for embedded current-carrying fields. The local pressure relation for the embedded field is a 3D Grad-Shafranov equation with finite-sheath solutions. The global relation reproduces the ambient MHD pressure equation without the embedded fields, but instead with the constraint that the ambient gas and magnetic pressures vary in proportion, as with the direct pressure balance. A coupled gas pressure in magnetically dominant regimes necessitates refilling outflows in a depleted atmosphere (actualized by flux-tube Lorentz forces) providing a compressively heated equilibrium corona with a specific global distribution of density, temperature, and steady accelerated outflow, all defined by the large-scale background magnetic field. Magnetic footpoint compression and twisting in a high-gas-pressure field-forming region (e.g. convection zone) outside, as below, the magnetically dominant regime, can introduce and sustain non-force-free embedded fields, thereby providing the energy for the coronal atmosphere. Such coronae may be relevant on very different astrophysical scales: around the sun and stars, and ranging from planets, to neutron stars, black holes, and spiral galaxies. Predicted coronal temperatures are corroborated.
L. November
Tue, 26 Mar 19
62/72
Comments: 25 pages, 3 figures