AN APPROACH TO THE FORMATION AND GROWTH OF NEW PHASES WITH APPLICATION TO POLYMER CRYSTALLIZATION - EFFECT OF FINITE-SIZE, METASTABILITY, AND OSTWALD RULE OF STAGES
A. Keller et al., AN APPROACH TO THE FORMATION AND GROWTH OF NEW PHASES WITH APPLICATION TO POLYMER CRYSTALLIZATION - EFFECT OF FINITE-SIZE, METASTABILITY, AND OSTWALD RULE OF STAGES, Journal of Materials Science, 29(10), 1994, pp. 2579-2604
This article aims to link the mainstream subject of chain-folded polym
er crystallization with the rather speciality field of extended-chain
crystallization, the latter typified by the crystallization of polyeth
ylene (PE) under pressure. Issues of wider generality are also raised
for crystal growth, and beyond for phase transformations. The underlyi
ng new experimental material comprises the prominent role of metastabl
e phases, specifically the mobile hexagonal phase in polyethylene whic
h can arise in preference to the orthorhombic phase in the phase regim
e where the latter is the stable regime, and the recognition of ''thic
kening growth'' as a primary growth process, as opposed to the traditi
onally considered secondary process of thickening. The scheme relies o
n considerations of crystal size as a thermodynamic variable, namely o
n melting-point depression, which is, in general, different for differ
ent polymorphs. It is shown that under specifiable conditions phase st
abilities can invert with size; that is a phase which is metastable fo
r infinite size can become the stable phase when the crystal is suffic
iently small. As applied to crystal growth, it follows that a crystal
can appear and grow in a phase that is different from that in its stat
e of ultimate stability, maintaining this in a metastable form when it
may or may not transform into the ultimate stable state in the course
of growth according to circumstances. For polymers this intermediate
initial state is one with high-chain mobility capable of ''thickening
growth'' which in turn ceases (or slows down) upon transformation, whe
n and if such occurs, thus ''locking in'' a finite lamellar thickness.
The complete situation can be represented by a P, T, 1/l(l = crystal
thickness) phase-stability diagram which, coupled with kinetic conside
rations, embodies all recognized modes of crystallization including ch
ain-folded and extended-chain type ones. The task that remains is to a
ssess which applies under given conditions of P and T A numerical asse
ssment of the most widely explored case of crystallization of PE under
atmospheric pressure indicates that there is a strong likelihood (cri
tically dependent on the choice of input parameters) that crystallizat
ion may proceed via a metastable, mobile, hexagonal phase, which is tr
ansiently stable at the smallest size where the crystal first appears,
with potentially profound consequences for the current picture of suc
h crystallization. Crystallization of PE from solution, however, would
, by such computations, proceed directly into the final stage of stabi
lity, upholding the validity of the existing treatments of chain-folde
d crystallization. The above treatment, in its wider applicability, pr
ovides a previously unsuspected thermodynamic foundation of Ostwald's
rule of stages by stating that phase transformation will always start
with the phase (polymorph) which is stable down to the smallest size,
irrespective of whether this is stable or metastable when fully grown.
In the case where the phase transformation is nucleation controlled,
a ready connection between the kinetic and thermodynamic consideration
s presents itself, including previously invoked kinetic explanations o
f the stage rule. To justify the statement that the crystal size can c
ontrol the transformation between two polymorphs, a recent result on 1
-4-poly-trans-butadiene is invoked. Furthermore, phase-stability condi
tions for wedge-shaped geometries are considered, as raised by current
experimental material on PE. It is found that inversion of phase stab
ilities (as compared to the conditions pertaining for parallel-sided s
ystems) can arise, with consequences for our scheme of polymer crystal
lization and with wider implications for phase transformations in tape
ring spaces in general. In addition, in two of the Appendices two them
es of overall generality (arising from present considerations for poly
mers) are developed analytically; namely, the competition of nucleatio
n-controlled phase growth of polymorphs as a function of input paramet
ers, and the effect of phase size on the triple point in phase diagram
s. The latter case leads, inter alia to the recognition of previously
unsuspected singularities, with consequences which are yet to be asses
sed.