A major mystery of glass-forming liquids is the non-Arrhenius
temperature-dependence of the average relaxation time. This paper briefly
reviews the classical phenomenological models for this phenomenon - the
free-volume model and the entropy model - and critiques against these models.
We then discuss a recent model [Dyre, Olsen, and Christensen, Phys. Rev. B 53,
2171 (1996)] according to which the activation energy for the average
relaxation time is determined by the work done in shoving aside the surrounding
liquid to create space needed for a flow event. In this model the non-Arrhenius
temperature-dependence is a consequence of the fact that the instantaneous
(infinite-frequency) shear modulus increases upon cooling.Comment: 18 pages, plain RevTex file, no figure