Jw. Nowok, VISCOSITY AND PHASE-TRANSFORMATION IN COAL ASH SLAGS NEAR AND BELOW THE TEMPERATURE OF CRITICAL VISCOSITY, Energy & fuels, 8(6), 1994, pp. 1324-1336
The phase transformation of multicomponent aluminosilicates on liquidu
s curves becomes an important parameter in the prediction of the slag
behavior upon cooling. Three major factors are taken into consideratio
n: (1) thermodynamic driving forces for a selection of stable phases o
n liquidus curves, such as free energies of components at various temp
eratures, (2) the effect of free energy of mixing on the tendency to p
hase segregation in liquid solution on cooling, and (3) free energy ch
ange at the solid-melt interface and entropy of fusion and their effec
ts on the morphology of the crystalline phase(s). In order to identify
the solid phase(s) crystallized from ash slag it is proposed, first,
to calculate major binary free energy composition diagrams based on ma
jor oxides in ash and, second, to select phase(s) with the free energy
and composition constrained by free energy diagrams. It is postulated
that the free energy of the solid-melt interface plays a significant
role in the selection of crystal size; the small Delta G(int) constrai
ns the formation of fine crystallites, while the large Delta G(int) in
dicates the formation of large crystals in a slag. It is quite apparen
t that the low Delta G(int) contributes to lowering the activation ene
rgy of nucleation. Both examples, the nucleation of fine crystallites
and the grwoth of large crystals, are evident in Beulah and Illinois N
o. 6 ash slags. In ash slags the phase transformation may occur either
by nucleation or by spinodal decomposition, both of which are recorde
d in Beulah and Gascoyne ash slags. The spinodal decomposition causes
a sharp increase of slag's viscosity. The differential thermal analysi
s (DTA) technique shows endotherms in Pittsburgh No. 8 and Gascoyne Wh
ite ash slags, on heating, near and above the temperature of critical
viscosity that are assigned to the dissolution of solid phases into th
e melt and anomalies in melt thermal conductivity, respectively.