Recent observations have shown that, rather than being uniform blocks
or clouds of cool material, solar prominences contain a great amount o
f fine structure in three dimensions. This model builds on a previous
model allowing variations in the two horizontal directions but now int
roduces variation in the vertical direction. The resulting prominence,
therefore, consists of a number of cool threads occupying dips in the
magnetic field. However, these cool fibrils are of differing vertical
extents i.e. some survive across a region of transition where the pro
minence geometry changes with height, while others exist only above or
below such a region. At the upper or lower edge of a fibril, the vert
ical extent of the dip is negatively correlated with the temperature i
.e. as the dip evens out, the temperature returns to coronal values. N
either the thermal nor the magnetic structure in the corona around the
prominence is influenced by the fibril structure within the prominenc
e.