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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.

    References

    1. N. Aubee, C. Dobbin, S. Marshall, T. Swabey,

    TAPPI 2004

    2. H. Hay, M. Weber, R. Donaldson, I. Gibbons, C.

    Bellehumeur, ANTEC 2004

    3. L. Mandelkern, J. Phys. Chem., 75, 3909 (1971)

    4. L. Mandelkern, Faraday Discuss. Chem. Soc., 68,

    310 (1979)

    5. L.E. Alexander, X-Ray Diffraction Methods in

    Polymer Science, Krieger Publishing Co., New

    York, 1979

    6. L. Mandelkern, M. Glotin and R.A. Benson,

    Macromolecules, 14, 22(1981)

    7. M. Glotin and L. Mandelkern, 14, 1394(1981)8. A. Lustiger, and N. Ishikawa, J. Polym. Sci., Part B,

    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.

    Ellison, J. Appl. Polym. Sci., 88, 545 (2003)

    14. A. Lustiger, Understanding Environmental Stress

    Cracking in Polyethylene, Medical Plastics andBiomaterials, July/August, 12(1996)

    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

    ANTEC 2005 /977