  The diverging relaxation time in approaching hypothetical ideal glass
transition is a subject of hot debate. In the current paper we demonstrate, how
diverging relaxation time and turning excess entropy to zero (which is an
essence of Kauzmann's paradox) can be avoided, using as an example the model
molecular glassformer, propylene carbonate. For this purpose we compare its
thermodynamic and dielectric relaxation properties, both known from the
literature. The agreement between two sets of data can be achieved, if we
suppose, that enthalpy of supercooled liquid propylene carbonate is governed by
activation law, and relaxation time follows double exponential law. We propose
the generalized Adam-Gibbs law to reconcile this two dependencies, and
qualitatively discuss its implications.
