We describe a model for the thermodynamics and dynamics of glass-forming
liquids in terms of excitations from an ideal glass state to a Gaussian
manifold of configurationally excited states. The quantitative fit of this
three parameter model to the experimental data on excess entropy and heat
capacity shows that ``fragile'' behavior, indicated by a sharply rising excess
heat capacity as the glass transition is approached from above, occurs in
anticipation of a first-order transition -- usually hidden below the glass
transition -- to a ``strong'' liquid state of low excess entropy. The dynamic
model relates relaxation to a hierarchical sequence of excitation events each
involving the probability of accumulating sufficient kinetic energy on a
separate excitable unit. Super-Arrhenius behavior of the relaxation rates, and
the known correlation of kinetic with thermodynamic fragility, both follow from
the way the rugged landscape induces fluctuations in the partitioning of energy
between vibrational and configurational manifolds. A relation is derived in
which the configurational heat capacity, rather than the configurational
entropy of the Adam Gibbs equation, controls the temperature dependence of the
relaxation times, and this gives a comparable account of the experimental
observations.Comment: 21 pp., 17 fig