Metastable states are not in true equilibrium and so cannot be directly tre
ated by thermodynamics and statistical thermodynamics. To circumvent this d
ifficulty one can specify an equivalent equilibrated state, equivalent in t
he sense that the observed macroscopic features are indistinguishable from
those of the metastable state, and equilibrated because of the imposition o
f auxiliary constraints which totally block the very slow relaxations that
cannot be completed during the time of the experiment. This procedure permi
ts one to treat metastable systems consistently within a completely time in
dependent and causal thermodynamic framework. It also gives a consistent de
scription of the entropy of glassy and similar random metastable systems in
which the entropy vanishes as T-->0 K, and it explains the apparent residu
al entropy at 0 K obtained in most conventional analyses based upon experim
ents carried out over irreversible paths (but not always recognized as such
).