We present a continuum theory of frustration-limited clusters in one-c
omponent glass-forming liquids that accounts, in part, for the recentl
y reported [Fischer et al., J. Non-Cryst. Solids, 131-133, 134 (1991)]
, and quite unexpected, presence in simple glass-forming liquids of st
able clusters at low temperatures (T) and the even less expected persi
stence for very long times of these clusters at higher Ts. The model i
s based on the idea that there is B local structure that is energetica
lly preferred over simple crystalline packing, which is strained (frus
trated) over large distances; although in a curved space the preferred
packing could lead to ''ideal'' crystallization at temperatures that
are usually above the actual freezing temperature, in ''flat'' space t
his transition is narrowly avoided. We are led to a new ansatz for the
T dependence of the viscosity, which permits us to collapse data for
many liquids onto a universal curve.