We investigate the transition of a two-dimensional electron gas from t
he regime of the quantum Hall effect to the regime of weak magnetic fi
elds for a tight-binding model. Unlike previous work, we find the foll
owing: (1) the linear field dependence of the extended-state energies
is not affected by disorder, although the total density of states belo
w each level of extended states increases with disorder strength; (2)
for each Landau band and disorder strength there exists a critical fie
ld B-c below which the extended level disappears, with B-c smaller for
lower Landau bands. We show how the experimental findings of level fl
otation and direct transition from high Landau level states to the And
erson insulating phase may be explained in light of our results.