We
provide a perspective on polymer glass formation, with an emphasis
on models in which the fluid entropy and collective particle motion
dominate the theoretical description and data analysis. The entropy
theory of glass formation has its origins in experimental observations
relating to correlations between the fluid entropy and liquid dynamics
going back nearly a century ago, and it has entered a new phase in
recent years. We first discuss the dynamics of liquids in the high-temperature
Arrhenius regime, where transition state theory is formally applicable.
We then summarize the evolution of the entropy theory from a qualitative
framework for organizing and interpreting temperature-dependent viscosity
data by Kauzmann to the formulation of a hypothetical “ideal
thermodynamic glass transition” by Gibbs and DiMarzio, followed
by seminal measurements linking entropy and relaxation by Bestul and
Chang and the Adam–Gibbs (AG) model of glass formation rationalizing
the observations of Bestul and Chang. These developments laid the
groundwork for the generalized entropy theory (GET), which merges
an improved lattice model of polymer thermodynamics accounting for
molecular structural details and enabling the analytic calculation
of the configurational entropy with the AG model, giving rise to a
highly predictive model of the segmental structural relaxation time
of polymeric glass-forming liquids. The development of the GET has
occurred in parallel with the string model of glass formation in which
concrete realizations of the cooperatively rearranging regions are
identified and quantified for a wide range of polymeric and other
glass-forming materials. The string model has shown that many of the
assumptions of AG are well supported by simulations, while others
are certainly not, giving rise to an entropy theory of glass formation
that is largely in accord with the GET. As the GET and string models
continue to be refined, these models progressively grow into a more
unified framework, and this Perspective reviews the present status
of development of this promising approach to the dynamics of polymeric
glass-forming liquids.