a theoretical investigation of the structure and function of mao (methylaluminoxane) eva zurek,...

32
A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Zurek, University of Calgary Al O O O Al Al Al O Al Al O O O O Al O Al Al Al Al O O O Al

Post on 20-Dec-2015

216 views

Category:

Documents


1 download

TRANSCRIPT

Page 1: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

A Theoretical Investigation of the Structure and Function of MAO

(Methylaluminoxane)

Eva Zurek, University of Calgary

AlO

O

OAl

Al

AlO

Al

Al

O

O

O

O

Al

O

Al

Al

Al

AlO

O

OAl

Page 2: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

Computational Details• DFT Calculations: performed with ADF 2.3.3 and 2000• Functional: LDA along with gradient corrected exchange functional of Becke;

correlation functional of Perdew• Basis-set: double- STO basis with one polarization function for H, C, Al, O; triple-

STO basis with one polarization function for Zr• Frequencies: single-point numerical differentiation • Molecular Mechanics: UFF2 parameterized to give entropies/enthalpies which agreed

with those obtained from ADF• Solvation: COnductor-like Screening Model (COSMO)• NMR Chemical Shifts: triple- STO basis with two polarization functions for H and C;

Gauge Including Atomic Orbitals (GIAO)• Transition States: geometry optimizations along a fixed reaction coordinate. TS where

gradient less than convergence criteria

Page 3: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

Catalysis

• K. Ziegler (1953) & G. Natta (1954); Nobel Prize in 1963

• Annual production of polyolefins is a hundred million tons (2001)

• 1/3 of the polymers made today are by Ziegler/Natta catalysis

• Polyethylene is the most popular plastic in the world

• Grocery bags, shampoo bottles, children’s toys, bullet proof vests (Kevlar), …

• Goal: to control MW, stereochemistry

• Single site catalysts: narrow MW distribution; higher stereoselectivity; higher activity

• Allow detailed structural & mechanistic studies

Page 4: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

Single-Site Homogeneous Catalysis

• Catalysts: L1L2MR1R2; L=Cp, NPR3, NCR2; M=Ti, Zr, R=methyl, propyl, etc.

• Co-Catalyst (Anion): B(C6F5)3, MAO (Methylaluminoxane)

• MAO + Cp2Zr(CH3)2 Cp2ZrCH3+ + MAOMe-

Zr+

CH3

Zr+

CH3

Zr+

CH3

Insertion Transition Stateπ-complexSeparated Species

Zr+

CH3

Product

C2H4, olefin

Page 5: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

MAODoes not crystallize

Gives complicated NMR

Industrially, one of themost important co-catalysts

MAO is formed from controlled hydrolysis of TMA (trimethylaluminum)

Why is an excess ofMAO necessary for

polymerization? (Al/Zr > 1000)

MAO is a ‘Black Box’

Page 6: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

‘Pure MAO’

• presence of different oligomers and multiple equilibria:

(AlOMe)x (AlOMe)y (AlOMe)z

• Experimental data suggests that x,y,z range between 9-30; 14-20

O

Al O

Al

Me

Me

O

Al

O

Al

O

Al

Me

MeMe

O

Al

O Al

O

Al

OAl

Me

Me

Me

Me

Cyclic Structures

Al

Me

OMe2AlO AlMe2

n

Linear Structure

O

Al

O

Al

O

Al

O

Al

O

Al

Al

O

Me

Me Me

MeMe

Fused Ring Structure

AlO

Al

OAl

O

AlO

Al

OAl

O

MeMe

Me

Me

Me

Me

Cage Structures

Page 7: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

• Three-dimensional cage structures, consisting of square, hexagonal and octagonal faces

• Four-coordinate Al centers bridged by three-coordinate O atoms

• [MeAlO]n, where n ranges between 4-16

• ADF calculations were performed on 35 different structures

Octagonal Face

Square Face

Hexagonal Face

Four-coordinate Al

Three-coordinate O

Four-coordinate Al

Three-coordinate O

Structural Investigation

Page 8: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

Constructing the Cages

Schlegel Diagram 3-D Representation

Page 9: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

• The order of stability is, 3H > 2H+S > H+O+S > 2O+S > 2H+O > 2S+H > 2S+O > 3S > 2O+H

• Structures composed of square and hexagonal faces only have the lowest energies for a given n

• SF = OF + 6

-2 octagonal; 8 square faces-16 atoms (2S+O) -Energy -6037.87kcal/mol

-2 octagonal; 8 square faces-4 (3S); 8 (2S+O); 4 (2O+S)-Energy -6028.60kcal/mol

-4 hexagonal; 6 square faces-8 (2S+H); 8 (2H+S)-Energy -6070.48kcal/mol

MAO Cage Energies

Page 10: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

Entropies & Enthalpies

• UFF2 (Universal Force Field) parametrized for (AlOMe)4 and (AlOMe)6

• Tested on two different (AlOMe)8 oligomers

• ZPE differs by up to 1.27 kcal/mol; entropy by up to 1.39 kcal/mol (298.15K)

Page 11: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

-755.00

-750.00

-745.00

-740.00

-735.00

-730.00

-725.00

4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30

n

Gibbs Free Energy Per Monomer (kcal/mol)

298.15

598.15

398.15

198.15

Gibbs Free Energy per (AlOMe) Unit

Page 12: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

0.00

5.00

10.00

15.00

20.00

4 6 8 10 12 14 16 18 20 22 24 26 28 30

n

Percentage

298.15398.15198.15598.15

Percent Distribution

average unit formula of (AlOMe)18.41, (AlOMe)17.23 , (AlOMe)16.89, (AlOMe)15.72 at 198K, 298K, 398K and 598K

Page 13: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

• Free TMA ((AlMe3)2) is always present in a MAO solution

• TMA and ‘pure’ MAO react with each other according to the following equilibrium

(AlOMe)n + m/2(TMA)2 (AlOMe)n•(TMA)m

• Difficult to measure amount of bound TMA. Estimates give Me/Al of 1.4 ~ 1.5

‘Real’ MAO

+1/2(TMA)2

ΔE = -13.06kcal/mol

Page 14: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

O: 3S

Al: 2S+H

O: 2S+H

Al: 3S

Variables Characterizing the Most Lewis Acidic

Site for (AlOMe)n

n Al environment O environment Bond Broken

6 2S+H 2S+H s-s

7 2S+H 3S s-s

8 2S+H 2S+H s-s

9 2H+S 2S+H s-h

10 2S+H 2S+H s-s

11 2S+H 2S+H s-s

13 2S+H 2S+H s-s

Reactive Sites in MAO

Page 15: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

ΔG(n,m) for Reaction of (AlOMe)n with m2

(TMA)2 at 298.15K

-10

-5

0

5

10

15

20

6 7 8 9 10 11 13

n

Δ ( , ) ( / )G n m kcal mol

1/2 ( )2TMA( )2TMA3/2 ( )2TMA2 ( )2TMA

Page 16: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

Temp (K) Me/Al AlTMA/Altot (%) Average Unit

Formula

% (AlOMe)12

198.15 1.00 0.21 (AlOMe)18.08•(TMA)0.04 15.27298.15 1.01 0.62 (AlO )Me 17.04•(TMA)0.11 19.05

398.15 1.02 1.05 (AlO )Me 15.72•(TMA)0.17 18.92

598.15 1.03 1.76 (AlO )Me 14.62•(TMA)0.26 16.56

• Most abundant species at every temperature still (AlOMe)12

• Increasing temperature shifts equilibrium towards slightly smaller structures

• Experimentally obtained ratio of Me/Al ~1.4 or 1.5 not obtained

Equilibrium Including TMA (1mol/L)

Page 17: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

+1/2(TMA)2

-14.17kcal/mol

-6.56kcal/mol

+

-23.15kcal/mol

+1/2(TMA)2

+

Interaction Between MAO, TMA and THF

Page 18: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

O

Al

O

Al

O

Al

Al

O

Al O

AlO

Al

O

Al

Al

O O

Al

O

AlO

AlO

Al

O

AlO O

Al

Al

O

Al

OO

Al

OAl

O

Al

Al

O

Al

O

Al

O

O Al

OAl

O

Al

OO

Al

Al

O

Al

O

O Al

AlO

Al

Al

OAl

OAl

O

Al

Al

O

Al

O Al

O

O

AlO

AlAl

O

O

Al

Al

O

OAl

Al

AlO

O

O

AlO

Al

OAl

O

AlO

Al

OAl

O

Al

O

Al

O

Al

OAl Al

OO

O

Al Al

O

Al

Al

Al

OO

Al

O O

(AlOMe)6 (AlOMe)7 (AlOMe)8

(AlOMe)9 (AlOMe)10 (AlOMe)11

(AlOMe)13

*

*

*

*

*

*

*

*

*

**

*

*

*

*

*

*

*

0.01%, 0.06% 0.01%, 0.00% 0.22%, 0.81%

1.22%, 2.22% 0.13%, 0.61% 2.36%, 1.17%

2.02%, 1.26%

Reactive MAO Cages

Page 19: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

• Species I: a weak complex

• Species II: binuclear complex contact ion-pair

• Species III: heterodinuclear complex contact ion pairs/similar separated ion pairs (possibly active)

• Species IV: unsymmetrically Me-bridged complex (possibly dormant)

ZrMe

MeIV

AlMAO

+

-

ZrMe

MeAl

Me

Me

III

MeMAO

+

-

ZrMe

Me

Zr

Me

II

MeMAO

+

-

ZrMe

MeI

AlMAO

‘Real’ MAO and Cp2ZrMe2

Page 20: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

Testing the Method

δexp δcalcΔδ

13C (Cp) 109.11 111.65 2.541H (Cp) 5.64 6.12 0.4813C (Me) 29.26 32.47 3.211H (Me) -0.15 -0.08 0.07

δexp δcalcΔδ

μ-Me 13C -5.34 -5.80 -0.46

μ-Me 1H -0.005 0.53 0.53

terminal 13C -8.025 -9.46 -1.44

terminal 1H -0.535 -0.64 -0.10

Chemical Shifts, ppm

Chemical Shifts, ppm

Page 21: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

δexp Integration exp δcalc Integration calc

13C (Cp) 112.0 10 115.83 101H (Cp) 5.7 10 6.67 1013C (Zr-Me) 29.5a) 1 42.33 11H (Zr-Me) - - 0.66 313C (μ-Me) 29.5a) 1 13.41 11H (μ-Me) - - 0.50 313C average* N/A N/A 27.87 2C1H average* N/A N/A 0.58 6Ha) only one band with double intensity revealed

* Corresponds to average chemical shift of Zr-Me and μ-Me for 13C

and 1H

The Weakly Interacting SpeciesChemical Shifts, ppm

Page 22: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

δexp Integration exp δcalc Integration calc

13C (Cp) 115.73 10C 113.60 10C1H (Cp) 5.5 10H 6.35 10H13C (Zr-Me) - - 41.7 1C1H (Zr-Me) - - 0.41 3H13C (μ-Me) 38.07 2C 19.38 1C1H (μ-Me) -0.27 6H 0.07 3H13C (Al-Me) -6.00 2C -1.21 2C1H (Al-Me) -0.58 6H -0.47 6H13C average* N/A N/A 30.54 2C1H average* N/A N/A 0.24 6H* Corresponds to average chemical shift of Zr-Me and μ-Me for 13C

and 1H

The ‘Active’ SpeciesChemical Shifts, ppm

Page 23: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

δexp Integration exp δcalc Integration calc

13C (Cp) 113.90 10 115.78 101H (Cp) 5.70 10 6.40 1013C (Zr-Me) 42.00 1 46.77 11H (Zr-Me) - - 0.38 313C (μ-Me) 9.00 1 - -1H (μ-Me) - - - -

The ‘Dormant’ SpeciesChemical Shifts, ppm

Page 24: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

+ Cp2ZrMe2

+ 1/2(Al2Me6)

-12.32 kcal/mol, t

-16.12 kcal/mol, t

-16.64 kcal/mol, t

0 kcal/mol

-13.06 kcal/mol, g

-16.88 kcal/mol, g

-16.58 kcal/mol, g

*g=gas phase t=toluene solution

+1/2 (Al2Me6)

Formation of ‘Dormant’, ‘Active’ Species

Page 25: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

Possible Mechanisms‘Dissociative’ Mechanism

‘Associative’ Mechanism

M+

π-complex

A-

M+

R

A-

M+

R

Insertion Transition State

Uptake TransitionState

Separated Species

A-

R

M+

A-

R

M+

π-complex

A-

RM+

R

A-

M+ R

A-

M+

A-

R

Insertion Transition State

Uptake Transition State

Separated Species

Page 26: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

First Insertion: ‘Dormant’ Species

Zr-O: 3.658

Zr-O: 4.539

Cis-Attack

Trans-Attack

Zr-O: 4.209

Zr-O: 3.336

Transition StateΔEgas= 38.80 kcal/molΔEtoluene= 35.55 kcal/mol

π-complexΔEgas= 31.88 kcal/molΔEtoluene= 28.43 kcal/mol

π-complexΔEgas= 34.65 kcal/molΔEtoluene= 26.96 kcal/mol

Transition StateΔEgas= 35.37 kcal/molΔEtoluene= 29.26 kcal/mol

Page 27: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

First Insertion: ‘Active’ Species

Cis-Attack

Trans-Attack

Zr-Me: 3.999 Zr-Me: 4.108

π-complexΔEgas= 20.73 kcal/molΔEtoluene= 16.22 kcal/mol

Transition StateΔEgas= 21.87 kcal/molΔEtoluene= 17.00 kcal/mol

Transition StateΔEgas= 16.63 kcal/molΔEtoluene= 18.36 kcal/mol

π-complexΔEgas= 14.97 kcal/molΔEtoluene= 12.32 kcal/mol

Zr-Me: 3.938 Zr-Me: 2.501

Page 28: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

Second Insertion: ‘Active’ Species

Transition StateΔEgas= 22.29 kcal/molΔEtoluene= 24.11 kcal/mol

Transition StateΔEgas= 21.26kcal/molΔEtoluene= 16.40 kcal/mol

π-complexΔEgas= 14.77 kcal/molΔEtoluene= 9.13 kcal/mol

Zr-Me: 2.517

Zr-Me:4.658

Page 29: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

Second Insertion: ‘Active’ Species

π-complexΔEgas= 18.70 kcal/molΔEtoluene= 13.69 kcal/mol

Zr-Me: 4.161

16.00

16.50

17.00

17.50

18.00

18.50

19.00

19.50

20.00

2.1 2.2 2.3 2.4 2.5 2.6 2.7 2.8

Cα-C ethylene ( )Distance Angstroms

(AlOMe)6(TMA)(Cp2ZrMeProp) + C2H4 Trans Attack; - agostic Interactions; Insertion Profile

Page 30: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

• In order for polymerization to occur, an excess of MAO is needed (typical conditions Al/Zr 1000 - 10,000)

• Most stable ‘pure’ MAO species do not contain strained acidic bonds and therefore do not react with TMA

• For example, (AlOMe)12, ~19% at 298.15 K

• [Cp2ZrMe]+[MeMAO]- is dormant

• [Cp2ZrMe]+[AlMe3MeMAO]- is active

• The same feature which makes a cage structure less stable is the same that makes it catalytically active!!!

Why is an Excess of MAO Necessary?

Page 31: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

Conclusions

• MAO consists of 3D cage structures with square and hexagonal faces

• Very little TMA is bound to ‘pure’ MAO; most exists as the dimer in solution

• Basic impurities in MAO can influence the equilibrium

• Identified most likely structures for ‘dormant’ and ‘active’ species in polymerization

• First insertion: cis-approach has an associated TS; trans-approach has a dissociated TS

• First insertion: trans-approach has lower insertion barrier

• Second insertion: trans-approach, α-agostic interaction has no insertion barrier. An uptake barrier needs to be found

Page 32: A Theoretical Investigation of the Structure and Function of MAO (Methylaluminoxane) Eva Zurek, University of Calgary

• Future Work: - to finish calculating uptake & insertion barriers for the second insertion; examine

termination barriers. Do the anion & cation associate after insertion?

• Acknowledgements:

- Tim Firman, Tom Woo, Robert Cook, Kumar Vanka, Artur Michalak, Michael Seth, Hans Martin Senn and other members of the Ziegler Research Group for their help and fruitful discussions

- Dr. Clark Landis, University of Wisconsin for giving us UFF2

- Novacor Research and Technology (NRTC) of Calgary ($$$)

- NSERC ($$$)

- Alberta Ingenuity Fund ($$$)

Miscellaneous