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SINGLE SITE CATALYSTS AND DUAL REACTOR TECHNOLOGY CREATE MORE
FREEDOM IN PE ROTOMOLDING RESIN AND PRODUCT DESIGNS
XiaoChuan (Alan) Wang, Mark Weber, Henry Hay, Marlee Cossar
NOVA Chemicals Corporation
Calgary, Alberta, Canada
Abstract
While polyethylene continues to be the resin of
choice for rotational molding, advancements in material
design are still required. From a structure-property
perspective, a thinner lamellar thickness of a polyethylene
resin may lead to a higher tie chain formation probability.
It is also believed that longer polymer chains with proper
comonomer incorporation enhance this probability. Single
site catalysts and octene comonomer usage enable the
design of rotomolding resins with superior propertiescompared with conventional Ziegler-Natta resins. This
paper combines our fundamental understanding of this
topic with experimental data.
Introduction
High performance octene polyethylene products
produced by single site catalysts (SSC) have been
discussed previously for high performance films [1], and
rotomolding products with enhanced processability [2].
With respect to rotomolding products, the objective of
this work is to provide more fundamental understandings
versus comparable Ziegler-Natta (ZN) hexenerotomolding resins.
It has been well known that for semi-crystalline
polyethylene, at least three phases must be considered to
describe its solid-state morphology, i.e., crystalline,
amorphous, and interfacial phases, as illustrated in Figure
1 [3,4,5,6,7]. Here, the interfacial phase is defined to be
that part of the non-crystalline material that represents a
transition zone between the surface of the crystal and that
point at which the presence of the crystal is no longer
significant in terms of affecting amorphous phase
molecular motion and conformation. This disordered
phase mainly includes loose chain loops, chain ends and
tie chains or molecules.It is widely believed that tie chains in
polyethylenes play key roles in affecting the end-use
physical properties such as toughness and environmental
stress crack resistance (ESCR). This is because tie chains
are the molecular chains connecting the lamellae together,
and their integrity is critical in order for the ductile-type
behavior to occur. Attempts have been made to infer the
relative amount of tie chains by experimental methods,
such as Fourier Transform Infrared Spectroscopy [8].
Calculation methods have also been suggested to infer the
information such as the tie chain formation probability
and relative concentration of tie chains, etc. [9, 10, 11].
However, the true quantity of tie chains has not been fully
confirmed by experimental results for a given resin and it
is expected to be very difficult from an experimental
perspective, although there have been some attempts to
correlate the experimental or calculated results with end-
use properties.
In this work, an experimental method has been
used to infer the relative amount of tie chains. From a
morphology point of view (Figure 1), the tie chains mustpass through the interfacial region. As a result, they may
be counted as part of the interfacial phase if measured by
an experimental method. With this fundamental
understanding in mind, for a similar polyethylene resin
category (e.g., roughly HDPE or MDPE), the measured
amount of the interfacial phase may be used as a relative
indication of the amount of tie chains, although not their
exact amount, since this phase includes at least loose
chain loops and chain ends as well. For this objective,
therefore, laser (514.5 nm) Raman spectroscopy internal
mode analysis of band intensities has been applied to
quantitatively characterize the polyethylene three-phase
structure, with respect to interfacial phase characterization
and hence the information about tie chains.
Experimental
Polymers and CharacterizationsThe solution octene HDPE and MDPE rotomolding resins
examined here were produced on a commercial plant
using NOVA Chemicals Advanced SCLAIRTECH
Technology and proprietary single site catalyst. The
bench mark hexene HDPE and MDPE rotomolding resins
were produced by a gas phase process and a Ziegler-Natta
catalyst. Analytical temperature rising elution
fractionation (A-TREF) fractions were obtained by ananalytical TREF system built in-house. Melt Index (MI or
I2) was measured in accordance with ASTM D-1238,
condition F (190oC/2.16kg). Density was obtained in
accordance with ASTM D-1505.
Polyethylene Three-Phase CharacterizationsRaman spectra were collected from a 514.5 nm laser
Raman Spectroscope at the Research Laboratory
Canmet Energy Technology Centre, Devon, Alberta,
Natural Resources Canada. The principle for using Raman
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technique to characterize the interfacial phase and hence
to infer the relative amount of tie chains is as follows.
Since the total integrated intensity Iref of the CH2twisting band at 1298 cm
-1is irrelevant to the
conformations of molecular chains, it can be used as an
internal intensity reference. The curve-fitting technique
was performed using Grams AI (Version 7.00). The totalintegrated intensity Iref at 1298 cm-1
was measured using
the integrate program in the Grams AI where the integrate
area from 1352 cm-1 to 1253 cm-1 was used. The band at
1416 cm-1
arises from crystalline regions. A curve fitting
program was used to obtain I1416 in which three peaks at
1461, 1442 and 1416 cm-1
were fitted in the area between
1550 cm-1
to 1400 cm-1
region using a 100% Gaussian
distribution and iterated until convergence. From the
integrated intensity of this band (I1416), the fraction of CH2units in the crystalline orthorhombic phase, or the
crystallinity of the sample can be calculated:
I
I
refc
46.0
1416=
(1)
where the constant 0.46 is measured from the spectrum of
fully crystalline polyethylene using 514.5 nm laser Raman
spectroscopy [12,13].
In the CH2 twisting vibration region, i.e., the
region of 1400 and 1250 cm-1
, a mixed 60% Gaussian and
40% Lorentzian curve-fitting program was used to obtain
I1303 in which the two peaks at 1303 cm-1
and 1298 cm-1
were fitted, the position of 1303 cm-1
was limited between
1303 cm-1
and 1305 cm-1
region and iterated until being
converged. The fraction of amorphous phase can then be
calculated:
I
I
ref
a
1303=
(2)
where the constant 1.0 is measured from the spectrum of
fully amorphous polyethylene using 514.5 nm laser
Raman spectroscope [12,13]. Finally, the mass fraction of
the interfacial region is given by:
acb = 1 (3)
Rotational Molding Trials and TestingThe resins were molded with a Ferry Industries
Inc. RS-160 rotational molding machine using
30.530.535.6 cm3
cast aluminum molds, under the
conditions of 5600F oven temperature and forced air
cooling. The oven time was changed to optimize the state
of cure and hence the physical properties. The impact
strength at 400C of the rotomolded part was evaluated
using the method recommended by the Association of
Rotational Molders (ARM) International. For the purpose
of this paper, only the maximum impact strength
achievable with 100% ductility (prior to the point where
the effects of possible thermal and oxidative
degradation/crosslinking are evident) is reported here and
will be explained below. The environmental stress crack
resistance of compression-molded plaques at constant
tensile load (abbreviated as CTL-ESCR) recommended byARM was evaluated at 300C, a stress level of 4.5 MPa,
20% notch depth, and 10% Igepal concentration.
Results and Discussion
Polymer Properties Table 1 shows the molecular
characteristics of the SSC and ZN rotomolding resins
examined in this paper. Two groups can be defined
according to the catalyst and comonomer type, i.e.,
SSC/octene (SSC-A and SSC-C) vs. ZN/hexene (ZN-B
and ZN-D). Note that within the same group (SSC-A vs.
SSC-C, and ZN-B vs. ZN-D), the change in weight
average molecular weight (Mw) is similar, in the range of
about 22000, and the molecular weight distribution
(MWD) remains relatively unchanged. Also note that the
SSC/octene resins have narrower molecular weight
distributions than their ZN/hexene counterparts (SSC-A
vs. ZN-B in HDPE resin category, and SSC-C vs. ZN-D
in MDPE resin category). It is well known that a
fundamental difference between a SSC and ZN resin is in
their comonomer distribution uniformity. A SSC resin has
a uniform comonomer distribution while that of a ZN
resin is heterogeneous. This is reflected by the
comonomer distribution breadth index (CDBI) measured
by A-TREF in Table 1. A higher value of CDBI is
indicative of a more homogeneous comonomerdistribution. Other molecular parameters being similar, it
is believed that a more uniform comonomer distribution
helps reduce the lamellar thickness and hence increases
the probability to form tie chains.
Three-Phase Measurements by Laser Raman As an
example, Figure 2 shows the de-convoluted crystalline
phase at the band of 1416 cm-1 in the crystalline
orthorhombic phase, and the de-convoluted amorphous
phase between the region of 1400 and 1250 cm-1
for ZN-
B. Table 2 summarizes the measured amounts of the
crystalline, amorphous and interfacial phases, and other
physical properties. It can be seen from Tables 1 and 2that for the comparable resins in the same resin category
(MDPE or HDPE), a SSC/octene resin has a comparable
or higher amount of the interfacial phase than its
ZN/hexene counterpart, even under the condition of
increased density or stiffness. This is significant, as one
would normally expect a smaller interfacial region for
resins with higher crystallinity, or density.
For the above two groups, comonomer distribution
uniformity and comonomer type have impacts on the
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amount of the interfacial phase. Recall that within the
same group (SSC-A vs. SSC-C, and ZN-B vs. ZN-D), the
change in Mw is similar, and MWD remains relatively
unchanged. It can been seen that, within the SSC/octene
resin group, an increase in octene content of 0.8 mol.%
results in a decrease in crystallinity (c) of 8.75 wt.%.
However, this trend is not so significant within theZN/hexene resin group, mainly due to its heterogeneous
comonomer distribution and hence reduced ability to
decrease crystallization. For example, within the
ZN/hexene group, an increase in a similar amount of
comonomer (0.9 mol.%, but it is hexene comonomer)
leads to only 5.0 wt.% reduction in crystallinity. Within
SSC/octene resin group, the amorphous (a) and
interfacial (b) amounts increase by 6.04 wt.% and 2.71
wt.% respectively, while for ZN/hexene resin group, the
increase in amorphous phase amount is similar (5.95
wt.%), however the interfacial amount seems to increase
by only 0.96 wt.%. Therefore, with the similar change in
comonomer content of about 0.8 mol.%, the change in the
amount of the interfacial phase within SSC/octene resin
group is about 2.8 times that within the ZN/hexene resin
group for the resins examined here. This is attributed to a
combination of the comonomer distribution uniformity of
a SSC resin, certain molecular species produced by the
multiple reactor process technology, and possibly the
longer chain length of octene comonomer.
Within either the HDPE or MDPE resin category in Table
2, why are higher amorphous contents (a) for these ZN
rotomolding resins observed? This is probably because
conventional ZN catalyst and its process technology
create more short polymer chains with many short chain
comonomer branches. A good example is in Figure 3 thatshows the analytical temperature rising fractionation
profiles for SSC-A and ZN-B. The weight fractions
between 25 to 900C elution temperatures are shown in
Table 2. It can be seen that ZN-B has a much higher
amount of chains with many branches that typically have
lower molecular weight. It is known that polyethylene
chains having comonomer branches normally do not enter
the tightly packed lamellar lattice. Depending on their
comonomer content and distribution, molecular weight
and crystallization conditions, these chains may enter
either amorphous or interfacial regions. For the
ZN/hexene group, the lower molecular weight molecules
with many branches seem to be concentrated mainly inthe amorphous phase, and this has be detected by laser
Raman spectroscopy.
Contrary to the ZN/hexene resin group, the use of single
site catalysts reduces the formation of those chains having
low molecular weight and many branches. As a result,
their amorphous region amount seems to be less if
compared with those of their ZN/hexene counterpart
examined here. Nevertheless, the higher molecular weight
of some species helps to increase the tie chain formation
probability. As a result, even with higher density or
stiffness, their interfacial phase amount and hence
probable amount of tie chains seem to be equivalent or
higher than their ZN/hexene counterparts. This increase in
tie molecules is anticipated to improve the inter-lamellar
failure resistance and be favorable to many physical
properties such as toughness at low temperature.
Meanwhile, it should be noted that the interfacial phase
also contains other species such as loose chain loops and
chain ends, in addition to tie chains. This has been hinted
by the data in Table 2. Therefore, the use of the interfacial
amount as a relative indication of tie chains should be
done with caution, preferably within the similar resin
category (e.g., HDPE or MDPE as an example here).
Toughness at low temperatures For a rotomolded
product, one of the key performance indicators is impact
strength at low temperatures. Table 2 contains the
maximum ARM impact strength (-400C) achievable with
100% ductility for the four resins examined. The rationalefor using this value is as follows. Assuming that the resins
are properly stabilized and the powders are fully sintered,
one may postulate that this value reflects more about the
intrinsic resin properties and hence the morphology.
Within the similar HDPE or MDPE resin category, it can
be seen that SSC-A and SSC-C have higher resin
densities and hence higher stiffness than ZN-B and ZN-D
respectively. For conventional commercial Ziegler-Natta
rotomolding products, typically the increase in stiffness
may lead to the subsequent decrease in toughness.
However, even with higher stiffness in the HDPE resin
category, the SSC/octene resin SSC-A appears to have
statistically (test error not shown here) equivalentmaximum impact strength compared to that of the
ZN/hexene resin ZN-B having lower stiffness. It is
believed that this is due to the increased amount of its
interfacial phase (b) and hence probably higher amount
of tie chains. This trend is further confirmed in the MDPE
resin category with the data of SSC-C. It has a much
higher density and hence stiffness than ZN-D.
Nevertheless, its higher interfacial amount or more tie
chains imparts a higher toughness than that for ZN-D, as
seen in Table 2.Environmental Stress Cracking Resistance Another
key performance indicator is environmental stress crackresistance (ESCR). Generally, environmental stress crack
resistance (ESCR) of polyethylene may be evaluated at
constant-strain tests (such as the bent-strip tests in ASTM
D 1693); and constant load testing under the tensile mode.
For the bent-strip test, there has long been a concern
about its ability to isolate the yield-stress (it actually
ought to be flexural modulus in the opinions of the
authors in this paper) property as a parameter independent
of the polymers stress-crack properties [14], since
different moduli of samples may result in different initial
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and persistant stress levels when subjected to such a test.
This can be understood from the test procedure. In the
bent strip test, samples are stressed by bending them into
a fixed-radius U-shape and holding them in place. Initial
stress levels are dependent upon the stiffness of the resin,
and long-term stress levels depend upon the creep
characteristics of the resin. For constant-tensile-load testswith an automatic failure-detection mechanism, specimen
stiffness also has a somewhat confounding effect, since
different stiffness may lead to a different deformation
under the constant load.
Although there has been some ambiguity with the
interpretation of ESCR results, it was surmised that
environmental stress cracking in polyethylene takes place
because of inter-lamellar failure, which in turn is caused
by relaxation of tie molecules [14]. It was further deduced
that the resistance to this failure mode can be best
reflected through constant-tensile-load testing, while
taking into account the differences in yield point among
various polyethylenes [14].
In this work (Table 2), it is found that the relationship of
the interfacial amount with either CTL-ESCR or
toughness at low temperature indeed seem to be in line
with the concept of an inter-lamellar failure mechanism,
when compared within the similar resin category.
Evidently, the higher interfacial amount and hence
possibly the increased number of tie chains for
SSC/octene resins seems to improve the ductile-brittle
transition in either low temperature impact testing or
constant-tensile-load ESCR testing, even under the
conditions of higher stiffness.
Conclusions
The amounts of the crystalline, amorphous and interfacial
phases for comparable single site/octene and Ziegler-
Natta/hexene rotomolding resins have been measured by
514.5 nm laser Raman spectroscopy. The results indicate
that the resins produced by single site catalyst and
multiple reactor process technology, in conjunction with
octene comonomer, seem to have higher interfacial
amount and hence possibly more tie chains even under the
conditions of higher density or stiffness, when compared
within the similar resin category. This possible increase in
the amount of tie molecules seems to improve the inter-lamellar failure resistance and is supported by the
experimental data, such as toughness at low temperature
and ESCR measured under a constant tensile load.
Compared with Ziegler-Natta/hexene counterparts, the
SSC/octene resins seem to have a better balance of higher
stiffness and equivalent or even higher toughness, while
meeting the practical needs in many rotomolding
applications.
Acknowledgements
The authors acknowledge NOVA Chemicals Corporation
for permission to publish this work.
Disclaimer
This information is furnished in good faith, without
warranty, representation, inducement or license of any
kind. All implied warranties and conditions (including
warranties and conditions of quality and fitness for a
particular purpose), are specifically excluded. No
freedom from infringement of a patent owned by NOVA
Chemicals or others is to be inferred.
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310 (1979)
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Polymer Science, Krieger Publishing Co., New
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Macromolecules, 14, 22(1981)
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Polym. Phys., 29, 1047(1991)
9. Y.L. Huang, and N. Brown, J. Polym. Sci., Part B,
Polym. Phys., 29, 129(1991)
10. R.M. Patel, K. Sehanobish, P. Jain, S.P. Chum, and
G.W. Knight, J. Appl. Polym. Sci., 60, 749 (1996)
11. R. Popli, and D. Roylance, Polym. Eng. Sci., 25(13),
828 (1985)
12. M. Failla, R.G. Alamo and L. Mandelkern, Polymer
Testing, 11, 151(1992)
13. R. P. Paradkar, S.S. Sakhalkar, X. He, and M.S.
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Keywords: tie chain, interfacial, amorphous,crystalline, Raman, single site, Ziegler-Natta, rotational
molding
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Table 1: Polymer Properties.
Table 2: Laser Raman Measurement Results, CTL-ESCR and ARM Maximum Impact Strength.
Figure 1: Illustration of Three-Phase Morphology of Polyethylene [3,4,5,6,7].
Figure 2: An Example of the Raman Spectra in the Crystalline and Amorphous Regions (ZN-B).
Figure 3: Comparison of Analytical Temperature-Rising Elution Fractionation Profiles of SSC-A and ZN-B.Resins.
0 . 0 0
0 . 0 5
0 . 1 0
0 . 1 5
0 . 2 0
0 . 2 5
2 0 3 0 4 0 5 0 6 0 7 0 8 0 9 0 1 0 0 1 1 0
T e ( C )
Absorbance
S S C - A , S S C / O c t e n e
Z N - B , Z N / H e x e n e
Catalyst
SSC-A HDPE SSC Octene 87500 2.19 0.3 90.9 0.944 1.7 129.4 187.3
ZN-B HDPE ZN Hexene 87000 2.90 0.8 51 0.942 1.8 128.6 174.5
SSC-C MDPE SSC Octene 64500 2.26 1.1 80.5 0.939 5.2 126.3 172
ZN-D MDPE ZN Hexene 66200 3.5 1.7 30 0.935 5 125.8 157.1
FTIR
Conomomer
content
(mol.%)
Resin
Category
H m(J/g)Sample Mw M w/M n CDBIComonomer DSC Tm
(oC)
Nominal
Density
(g/cm3)
M I
(dg/min.)
SSC-A HDPE SSC Octene 7.1 71.59 13.64 14.77 240 235 990 23.5
ZN-B HDPE ZN Hexene 28.7 68.4 18.74 12.86 280 254 920 21.1
SSC-C MDPE SSC Octene 41.5 62.84 19.68 17.48 110 202 750 19.9
ZN-D MDPE ZN Hexene 43.3 63.41 24.69 11.9 87 160 620 17.4
Resin
Category
Catalyst CTL-
ESCR
(hrs)
Max
ARM
Impact
(J)
Sample Comonomer A-
TREF
(< 900C
fraction
a
(wt.%)
c
(wt.%)
b
(wt.%)
Tensile
Yield
Stress
(MPa)
1%
Flexural
Modulus
(MPa)
Z N - B
C r y s t a l l in e
P h a s e
A m o r p h o u s
P h a s e
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