Recall that in the region below the photosphere, convective cells are largely responsible for vertical motion of large packets of gas and that this bubbling activity carries heat from the interior to the solar surface. Magnetic fields exert forces on charged particles and, because this solar material is highly ionized, the magnetic fields influence the convective motion. Detailed considerations indicate that the magnetic forces hinder the convection of heat to the surface by making it harder for the hot gases to rise. Thus, the region in sunspots having strong magnetic fields tends to be cooler than the surrounding region and appears darker than the surrounding regions at higher temperature.
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As the Sun rotates, because the equator rotates faster the lines of the magnetic field get distorted. Over many rotations, this has the effect of wrapping the field lines multiple times around the Sun. Sunspot pairs then develop when these wrapped field lines tangle because of underlying convective motion and penetrate the surface in loops.
In this interpretation, prominences (which are great loops above the solar surface) are just such loops between sunspot pairs seen on the limb of the Sun against the blackness of space. Later we will see that eruptions from the solar surface (flares) probably result from loops in the field lines that reconnect suddenly, releasing large amounts of energy.
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Further, when this happens the magnetic field reverses its polarity; this
explains the alternating magnetic polarities of sunspot pairs in successive cycles. This also explains the twenty-two-year
magnetic cycle: it takes two successive eleven-year sunspot cycles, one with one polarity and the next with reversed
polarity before returning to the original polarity. Thus the full Babcock cycle is twenty-two years.