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Free energy density of a system that can undergo a phase transition as a function of an order parameter. Curves a, b, c correspond to different temperatures: (a) T C <T<T E , (b) T= T E , (c) T> T E . Only b curve is possible for continuous transitions.  

Free energy density of a system that can undergo a phase transition as a function of an order parameter. Curves a, b, c correspond to different temperatures: (a) T C <T<T E , (b) T= T E , (c) T> T E . Only b curve is possible for continuous transitions.  

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All stages of phase transformations in materials, nucleation, growth, and coarsening, are subjected to thermal effects that stem from the redistribution of energy in the system like, release of latent heat and heat conduction. The thermal effects change the rate and outcome of the transformation and may result in appearance of unusual states or pha...

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Context 1
... equilibrium states η E =Ξ(T) are the extremals of the free energy functional, Eq.(2). The homogeneous part of the equilibrium set η E =Ξ(T) must have at least two minima, η 1 and η 2 , corresponding to stable phases, separated by a maximum, which corresponds to an unstable equilibrium state, η t , called transition state, Figure 1. A few important parameters may be defined for the system: the equilibrium temperature T E -as f(T E , η 1 )= f(T E , η 2 ); the activation barrier height B=f(T E , η t )-f(T E , η 1 ); and the latent heat L=|e(T, η 1 )-e(T, η 2 )| of transformation. ...
Context 2
... discontinuous transitions b≠0 and the equilibrium set η E =Ξ(T) consists of phases with different symmetries, disordered with η α =0 and ordered with η β (T), separated by the transition state η γ (T), which is unstable above T C but gains thermodynamic stability below T C , Figure 2b. The activation barrier B exists at all temperatures above the spinodal one, see Fig.1, the latent heat L does not vanish, and, in accordance with the Gibbs phase rule, the thermodynamic equilibrium between β and α phases is achieved at the specific temperature T E only, see Fig.2b. ...
Context 3
... (16, 17) identify the local interfacial variables V n , K, T_, [T], [dT/du], and relate them to the thermodynamic interfacial quantities, L, σ, ε, Γ s , l I and kinetic properties of the medium like α, m. The beauty of these equations is that they are expressed only through measurable quantities and appropriate thermodynamic parameters of a system and still are applicable to many different situations. ...
Context 4
... interesting and unusual equilibrium thermal effect consists in stabilization of the transition state γ in very small particles of materials that undergo discontinuous transitions. The most striking feature of this effect is that the transition state possesses maximum free energy among all other homogeneous states of the system at the same temperature, see Fig.1. This state was called the adiabatic nanophase (ANP) [17] because stabilization of the transition state is a completely equilibrium effect, which comes about as a result of two mutually assisting constraints: insulation and confinement. ...

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