Fig. 6

Evolution of the Lyα (blue lines) and UV continuum (red) escape
fraction as a function of the dust optical depth
()
for a homogeneous (triangles), a weakly clumpy (squares), and an extremely clumpy
(spheres) medium. In these simulations, we adopt FF = 0.23, CF = 0.997
(Rmin = 49 and Rmax = 64
cells),
= 1019 cm-2, vexp = 0
km s-1, and b = 40 km s-1. For
comparison, the UV escape fractions (Fig. 4) are overlaid (red lines). For the
extremely clumpy medium we note that for
larger than a certain limit τc (here roughly equal to
3.5), fesc(UV) drops below
fesc(Lyα).
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