Fig. 6

The “sunspot” like magnetic field configuration used in the long-term integration
numerical test. On the left panel we plot the ratio of the local
Alfvén to the sound speed as a function of x and
z. The magnetic field becomes dynamically unimportant in the deeper
layers because the background hydrostatic pressure increases with relative rapidity.
The right panel displays a horizontal cut (at the solar
photosphere) through the fast mode speed ().
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