Abstract:
Interfaces are ubiquitous in natural phenomena. While the description of interfaces in
fluid systems is well developed, solid-fluid and solid-solid interfaces are not well understood.
This deficiency is especially true for solid-solid interfaces, which play critical roles in materials
engineering, solid-state physics and solid-state chemistry. In this thesis, the Gibbs
theory of interfaces is generalized to describe phase boundaries under non-hydrostatic stress
in multicomponent systems. We obtain equations that describe coherent solid-solid interfaces
with shear stresses parallel to the boundary plane, incoherent solid-solid interfaces for
certain constraint variations, solid-fluid interfaces, grain boundaries and surfaces.
In the second part of the thesis, the developed theory is applied to study particular types
of interfaces using atomistic simulations. We modeled solid surface, solid-liquid interface
and grain boundaries. The simulations allowed to calculate values of key thermodynamic
properties, clarify behavior of these properties with temperature, composition and stress
and test the predictions of the theory.
Surface surface free energy and surface stress in a single component system were computed
as functions of temperature. The values of these two excess properties do not converge
near the melting point despite the extensive surface premelting.
Solid-liquid interface free energy was computed using the developed thermodynamic
integration technique as a function of composition in CuAg binary alloy and as a function
of biaxial strain in a single component Cu system. In the later case the equilibrium states
between the non-hydrostatically stressed solid and liquid were accurately predicted using the
derived Clausius–Clapeyron type equation. We show that for non-hydrostatic equilibrium
interfaces stress is not unique and compute different interface stresses using our simulation
data.
We also studied effects of elastic deformation, temperature and chemical composition
on properties of a symmetrical tilt grain boundary in Cu and CuAg alloy. Excess grain
boundary free energy was computed as a function of lateral strain, normal stress and shear
stress parallel to the boundary plane. We also employed the derived thermodynamic integration
method to compute grain boundary free energy as a function of temperature and
composition. Maxwell type relations predicted by the adsorption equation were tested and
verified.
We proposed a thermodynamic model of liquid nucleation on superheated grain boundaries
based on the sharp-interface approximation with a disjoining potential. The model
predicts the shape and size of the critical nucleus by using a variational approach. Contrary
to the classical nucleation theory, the model predicts the existence of a critical temperature
of superheating and offers a simple formula for its calculation. The model is tested
against molecular dynamic simulations in which liquid nuclei at a superheated boundary
were obtained by an adiabatic trapping procedure.