Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
10271618 | Fluid Phase Equilibria | 2005 | 7 Pages |
Abstract
The discontinuous changes of volume ÎVm, entropy ÎSm and heat capacity at constant pressure ÎCP, m at the melting point have been predicted by the Landau theory of phase transition where the Gibbs free energy Φ in order state is expressed by Φ = Φ0 + Aη2 â Cη4 + Eη6, where η is an order parameter. In this work, A is given by a function that A = k0(T â T0)m(P0 â P)n, where k0, m, n, T0, and P0 are constants. The order parameter ηmin for the minimum of Φmin is related to the volume of solid Vs and is expressed by:CA*2ηmin4â38CA*3ηmin6=1âÎVÎVmwhere ÎV = Vs â Vm, s, ÎVm = Vm, l â Vm, s and A* is the value of A at the melting point. The volume of Vs changes from Vm, s to Vm, l, where ÎVm, s and ÎVm, l are volumes of solid and liquid phases at the melting point, respectively. The discontinuous change of thermal pressure coefficient γv = (âP/âT)V, thermal expansion (âV/âT)P and compressibility â(âV/âP)T at the melting point has been calculated. A typical function of Φ for a polymer has been demonstrated as a function of η and C at the melting transition.
Related Topics
Physical Sciences and Engineering
Chemical Engineering
Chemical Engineering (General)
Authors
S. Saeki,