  A continuum model of crystalline solid equilibrium is presented in which the
underlying periodic lattice structure is taken explicitly into account. This
model also allows for both point and line defects in the bulk of the lattice
and at interfaces, and the kinematics of such defects is discussed in some
detail. A Gibbsian variational argument is used to derive the necessary bulk
and interfacial conditions for multi-phase equilibrium (crystal-crystal and
crystal-melt) where the allowed lattice variations involve the creation and
transport of defects in the bulk and at the phase interface. An interfacial
energy, assumed to depend on the interfacial dislocation density and the
orientation of the interface with respect to the lattices of both phases, is
also included in the analysis. Previous equilibrium results based on nonlinear
elastic models for incoherent and coherent interfaces are recovered as special
cases for when the lattice distortion is constrained to coincide with the
macroscopic deformation gradient, thereby excluding bulk dislocations. The
formulation is purely spatial and needs no recourse to a fixed reference
configuration or an elastic-plastic decomposition of the strain. Such a
decomposition can be introduced however through an incremental elastic
deformation superposed onto an already dislocated state, but leads to
additional equilibrium conditions. The presentation emphasizes the role of
{configurational forces} as they provide a natural framework for the
description and interpretation of singularities and phase transitions.
