APS March Meeting 2016
Volume 61, Number 2
Monday–Friday, March 14–18, 2016;
Baltimore, Maryland
Session V42: Polymer Architecture, Control of Structure and Dynamics in Polyolefins
2:30 PM–5:30 PM,
Thursday, March 17, 2016
Room: 345
Sponsoring
Unit:
DPOLY
Chair: Lin Wang, The Dow Chemical Company
Abstract ID: BAPS.2016.MAR.V42.1
Abstract: V42.00001 : Melt structure and self-nucleation of ethylene copolymers*
2:30 PM–3:06 PM
Preview Abstract
Abstract
Author:
Rufina G Alamo
(Florida State University, FAMU-FSU College of Engineering, Tallahassee, FL 32310 USA)
A strong memory effect of crystallization has been observed in melts of
random ethylene copolymers well above the equilibrium melting temperature.
These studies have been carried out by DSC, x-ray, TEM and optical
microscopy on a large number of model, narrow, and broad copolymers with
different comonomer types and contents. Melt memory is correlated with
self-seeds that increase the crystallization rate of ethylene copolymers.
The seeds are associated with molten ethylene sequences from the initial
crystals that remain in close proximity and lower the nucleation barrier.
Diffusion of all sequences to a randomized melt state is a slow process,
restricted by topological chain constraints (loops, knots, and other
entanglements) that build in the intercrystalline region during
crystallization. Self-seeds dissolve above a critical melt temperature that
demarcates homogeneity of the copolymer melt. There is a critical threshold
level of crystallinity to observe the effect of melt memory on
crystallization rate, thus supporting the correlation between melt memory
and the change in melt structure during copolymer crystallization. Unlike
binary blends, commercial ethylene-1-alkene copolymers with a range in
inter-chain comonomer composition between 1 and about 15 mol {\%} display an
inversion of the crystallization rate in a range of melt temperatures where
narrow copolymers show a continuous acceleration of the rate. With
decreasing the initial melt temperature, broadly distributed copolymers show
enhanced crystallization followed by a decrease of crystallization rate. The
inversion demarcates the onset of liquid-liquid phase separation (LLPS) and
a reduction of self-nuclei due to the strong thermodynamic drive for
molecular segregation inside the binodal. The strong effect of melt memory
on crystallization rate can be used to identify liquid-liquid phase
separation in broadly distributed copolymers, and offers strategies to
control the state of copolymer melts in ways of technological relevance for
melt processing of LLDPE and other random olefin copolymers.
References:
B. O. Reid, et al, Macromolecules 46, 6485-6497, 2013
H. Gao, et al, Macromolecules 46, 6498-6506, 2013
A. Mamun et al, Macromolecules 47, 7958-7970, 2014
X. Chen et al, Macromol. Chem. Phys. 216, 1220$-$1226, 2015
M. Ren et al, Macromol. Symp. 356, 131--141, 2015
*Work supported by the NSF (DMR1105129)
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2016.MAR.V42.1