Image Details
Caption: Figure 1.
Illustration of the formation and evolution of a simple bipolar AR from the emergence of an isolated magnetic flux tube. The local photospheric surface is shown as a gray transparent plane. Panel (a) summarizes graphically the evolution of magnetic flux (green color) over the lifetime of the bipolar AR. Initially (after the onset of emergence, tstart; panel (c)), the two opposite polarities (N and P) form a PIL and self-separate rapidly (separation distance and speed are overplotted as black and white curves, respectively). The self-separation of opposite flux progressively slows down until the end of the flux emergence phase, where the bipole has assumed its final (typically maximum) self-separation at the surface (tend; panel (d)). The decay phase begins (tdecay; panel (e)) when surface effects spread and transport the flux from the initially compact polarity concentrations and lead them to cancel out and submerge at the PIL, leading to a reduction of flux observed at the surface.
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