In the present work the application of the Johnson-Mehl-Avrami-Kolmogo
rov (JMAK) theory for the calculation of the volume fraction crystalli
zed is discussed for several particular cases of isothermal transforma
tions. In particular, the following three situations, for which the JM
AK theory requires extensions, are considered: (1) finite size effects
and non-uniform nucleation, (2) anisotropic particle formation, and (
3) transient nucleation. We present new equations which describe these
three situations. In general, we find that anisotropic particle forma
tion, finite size effects and non-uniform nucleation lead to a reducti
on of the crystallization rate. Furthermore, transformations which pro
duce anisotropic particles are characterized by reduced values of the
Avrami exponents. Finally, we demonstrate that corrections to the JMAK
t(4) law arising from time dependent nucleation must include size-dep
endent growth effects to obtain a logically consistent result. (C) 199
7 Elsevier Science B.V.