In this paper we develop conditions that govern the evolution of a ful
ly faceted interface separating elastic phases. To focus attention on
the effects of elastic stress, we restrict attention to interface-cont
rolled kinetics, neglecting bulk transport; and to avoid geometric com
plications, we limit our discussion to two space-dimensions. We consid
er a theory in which the orientations present on the evolving particle
are not necessarily those given by the Wulff shape: we allow for meta
stable crystallographic orientations as well as stable orientations. W
e find that elastic stress affects the velocity of a facet through the
average value of the normal component of the jump in configurational
stress (Eshelby stress) over the facet. Within our theory singularitie
s in stress induced by the presence of corners do not influence the ve
locity of the facet. We discuss the nucleation of facets from corners;
the resulting nucleation condition is shown to be independent of elas
tic stress. We also develop equations governing the equilibrium shape
of a faceted particle in the presence of elastic stress.