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Modeling MAO (Methylalumoxane)

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Title: Modeling MAO (Methylalumoxane)


1
Modeling MAO (Methylalumoxane)
  • Eva Zurek, Tom Woo, Tim Firman, Tom Ziegler
  • University of Calgary, Department of Chemistry,
    Alberta, Canada, T2N-1N4

2
Introduction
  • MAO is one of the most industrially important
    activators in single-site metallocene catalyst
    polymerization
  • Commonly accepted role of MAO in
    catalysis ?(n5-C5H5)2ZrMe2 MAO ?
    (n5-C5H5)2ZrMe (MAO)Me-
    ?(n5-C5H5)2ZrMe nCH2CH2 ?
    (n5-C5H5)2Zr-CH2-CH2n-CH3
  • Not possible to isolate crystalline samples of
    MAO disproportionation reactions give
    complicated NMR spectra
  • Hence, it is not possible to characterize MAO and
    thus the structure(s) of MAO remain largely
    unknown
  • Goal of study is to propose a structural model
    for MAO

3
Preliminary Structural Investigation
  • Density Functional Theory Calculations were
    carried out using the Amsterdam Density
    Functional (ADF) program version 2.3.3
  • Binding Energy Per Monomer (E(AlOMe)n -
    En(AlOMe))/n
  • Preliminary study shows that three-dimensional
    caged structure have lower BE/monomer, thus are
    more energetically stable than two-dimensional
    sheet structures

4
Types of Structures Studied
  • Three-dimensional cage structures, consisting of
    square, hexagonal and octagonal faces
  • Four-coordinate Al centers bridged by
    three-coordinate O atoms
  • MeAlOn, where n ranges between 4-16
  • ADF calculations were performed on 35 different
    structures

5
Mathematical Relationships
  • For a given MAO Structure the following
    mathematical relationships were derived
  • SF OF 6 1
  • 3(3S) 2(2SH) (2HS) 24 2
  • (2SH) 2(2HS) 3(3H) 6(HF) 3
  • SF is of square, HF is of hexagonal, OF is
    octagonal faces
  • (3S) is the of atoms bonded to three square
    faces, (2SH) the number of atoms bonded to two
    square and one hexagonal face, etcetera.
  • 1 shows us that minimum number of SF in MAO
    cage is 6, when OF is zero
  • 2 and 3 can be used to construct large MAO
    cages with OF zero using concepts from
    Regular Polytopes, the branch of Pure Mathematics
    which studies Polyhedrons in n-dimensions


6
Formula for Predicting MAO Cage Energies/ Example
Shown for (AlOMe)8
  • A least squares fit was performed to derive a
    formula predicting MAO Energies
  • E -373.57(3S) -377.49(2SH) -381.13(2HS)
    -381.80(3H) -377.14(2SO) -380.59(2OS)
    -381.03(SOH) -378.86(2HO) -365.51(2OH)kcal/mol
  • Rms deviation was found as being 4.70kcal/mol for
    35 structures

7
Determination of Entropic/Enthalpic Corrections
  • ADF Frequency calculations on (AlOMe)4 and
    (AlOMe)6 were used to parametrize UFF 2
    (Molecular Mechanics Program)
  • Parametrization gave good values for two
    different (AlOMe)8 isomers
  • This parametrized version of UFF2 was then used
    to calculate entropies and finite temperature
    enthalpy corrections for the 35 different MAO
    structures

8
Enthalpic Considerations
  • Equations were found which predict enthalpic
    values for (AlOMe)n
  • H0 25n kcal/mol 5
  • Vibrational Portion of Htemp 6 Hvib
    H0 (0.0028T - 0.3548)n x ln(T) rms
    deviation of 3.28, 0.78, 1.32 and 3.36kcal/mol at
    198.15K, 298.15K, 398.15K, 598.15K
  • H E H0 Htemp 4 where E
    is the energy, H0 the zero-point energy, Htemp
    the finite temperature enthalpy correction

9
Entropic Considerations
  • Svib 7.91(3S)8.30(2SH)10.20(2HS)8.49(3H)10
    .41(2SO)9.50(2OS)10.45(SOH)7.32(2H
    O)0(2OH) cal/molK
    9 rms deviation of
    1.78Kcal/mol at 298.15K
  • Extension to Different Temperatues
  • Translational Entropy 10
    S2 S1 T2/T1 T2(0.014) - 5.47
  • Rotational Entropy 11 S2
    S1 T2/T1 T2(0.007) - 3.28
  • Vibrational Entropy 12 S2
    (T2/T1-((0.0006T22 - 0.5353T2 108.85)-1)S1
    rms deviation of 0.27, 1.70 and
    4.90kcal/mol at 198.15K, 398.15K, 598.15K
  • Strans (0.35n 41.17)cal/molK at 298.15K
    7
  • Srot (0.57n 30.57)cal/molK at 298.15K
    8

S Svib Strans Srot
10
Gibbs Free Energy Per Monomer (AlOMe unit) at
Different Temperatures (G/n)
  • Lowest Gibbs Free Energy per Monomer Unit gives
    most stable structure
  • For a given n, the most stable structures
    composed of SF and HF only. Reason equation 1
    shows that as OF increases, so does SF. SF
    exhibit ring strain therefore destabilizing the
    structure
  • Graph shows G/n for structures composed of SF and
    HF only
  • Equations 2 and 3 used to construct
    structures for n gt 16.
  • Equations 4 - 11 used to predict G/n for n
    14 n gt 16.
  • Most Stable structure at all temperatures is
    (AlOMe)12
  • At low temperatures, (AlOMe)16 is almost as
    stable as (AlOMe)12

DG DE DH0 D Htemp -T D S
11
Percentage of Each n at Different Temperatures
  • Most stable structure is (AlOMe)12
  • Consists of 24 atoms in a (2HS) environment
    6SF 8HF
  • t-butyl analogue sunthesized by Barron and
    co-workers 1,2
  • Graph corresponds to experimental data, which
    predicts that n ranges between 9 and 30 3 and
    between 14 and 20 4

12
Investigation of MAO-TMA Interactions
  • All MAO solutions contain residual TMA
    (trimethylaluminum)
  • It has been shown that TMA participates in
    equilibrium with different MAO oligomers2 and in
    disproportionation reactions5
  • The way in which TMA bonds to MAO was determined
    via studying (AlOMe)6
  • (AlMe)2 bonds to the oxygen and there is an Me
    transfer to the Al
  • The bond which breaks belongs to two square faces
    and both the Al and O are in a (2SH) environment

13
Determining the Sites with Greatest Latent Lewis
Acidity
  • The bond which gives us the greatest DE value
    when reacted with TMA has the greatest Latent
    Lewis Acidity (LLA). Bonds with greatest LLA for
    structures composed of SF and HF only are shown
    below
  • The figure below shows us that LLA is dependant
    upon the presence of SF
  • Equation 1 shows that for a MAO structure
    composed of SF and HF, there are only six SF
    present hence there are few LLA sites
  • Cp2ZrMe2 also coordinates to the LLA sites in
    MAO, and hence there are a limited amount of
    sites where this could occur. This explains the
    high AlZr ratio needed for catalysis to occur.

14
Conclusions
  • Formulae predicting the energy, entropy and
    finite temperature enthalpy corrections for a
    given MAO structure consisting of SF, HF and OF
    have been found
  • When pure MAO is considered (AlOMe)12 is the most
    stable structure in the temperature range
    198.15K-598.15K
  • The way in which TMA bonds to MAO has been
    determined
  • The sites exhibiting greatest LLA for five MAO
    structures have been found
  • It has been shown that the presence of LLA is
    dependant upon the presence of SF
  • The high ratio of AlZr which is needed for
    catalysis to occur is attributed to the limited
    amount of SF present within a MAO structure (cf.
    Equation 1)

15
Miscellaneous
  • Acknowledgements Dr. Clark Landis,
    University of Wisconsin for supplying us with
    UFF2 NSERC
  • References 1) Mason, M.R. Smith, J.M.
    Bott, S.G. Barron, A.R. J. Am. Chem. Soc. 1993,
    115, 4971. 2) Harlan, C.F. Mason, M.R. Barron,
    A.R. Organomet. 1994, 13, 2957. 3) Babushkin,
    D.E. Semikolenova, N.V. Panchenko, V.N.
    Sobolev, A.P. Zakharov, V.A. Talsi, E.P.
    Macromol. Chem. Phys. 1997, 198, 3845. 4)
    Talsi, E.P. Semikolenova, N.V. Panchenko, V.N.
    Sobolev, A.P. Babushkin, D.E. Shubin,
    A.A. Zakharov, V.A. J. Molecular Catalysis A
    Chemical, 1999, 139, 131. 5) Tritto, I. Sacchi,
    M.C. Locatelli, P. Macromol. Chem. Phys. 1996,
    197, 1537.
  • Work in Progress -to study the role which
    TMA plays in lowering the energeies of different
    MAO oligomers -to study the metallocene/MAO
    interaction thereby determining the active
    species in polymerization
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