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Scientific Computing & Modelling, Chemistry Department, Vrije Universiteit, De Boelelaan 1083, 1081 HV Amsterdam, The Netherlands
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14344274910
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note
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In some experiments, the average polymerization temperature was somewhat higher than the thermostat setting (see Tables 1-3), in particular, with the high-yield catalysts.
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32
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0001268540
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34
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14344267930
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note
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The effect of preactivation was also studied in ref 22. Also in this work, no effect of preactivation time on the shape of the activity-time profile could be observed.
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35
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14344279037
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note
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Except run 272 where a higher Zr concentration was used (see Table 1).
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36
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14344275106
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note
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2/MAO.
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37
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14344279995
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note
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n and the amounts of unsaturations. This allows for estimates of activation energy differences based on the plots in Figure 8.
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38
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14344271096
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A misprint in Table 3 in ref 6 has been corrected in: Thorshaug, K.; et al. Macromolecules 1998, 31, 9416.
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14344282956
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note
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2, containing two methyl bridges between Zr and Al. Certainly, such a complexation with TMA (which is always present to some extent in a MAO cocatalytic solution) will also slow insertion of the first monomer. However, the metalligand agostic interaction represents an additional effect that makes the catalysts with R = Et and longer qualitatively different from the catalysts with R = H or R = Me.
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46
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14344285306
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note
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R interaction with R = Bu than with R = n-Pr is in agreement with our previous experience, namely that a hydrogen atom on a secondary carbon forms a stronger agostic bond than one on a primary carbon.
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47
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14344268138
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note
-
3 (i.e., without a metal-ligand agostic interaction) confirm this picture: 0.736, 0.658, 0.656, and 0.654 for R = H, Me, Et, and n-Pr, respectively. Apparently, the insertion barrier is not affected accordingly. The exact values of the insertion barriers in these systems depend on the choice of gradient corrections to the density functional. In ref 6, we found barriers of 26 and 10 kJ/mol for the first and second insertion with R = H, using so-called BLYP gradient corrections. With the BP91 gradient corrections used in the present work, the corresponding insertion barriers are 4 and 0 kJ/mol. In both cases, the first insertion has the highest energy barrier.
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48
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14344277935
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note
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The insertion product after passing through an α-agostic transition state has an agostic bond between Zr and γ-H on the growing polymer chain. Therefore, γ-agostic conformaj tions were chosen as the basis for the QSAR analysis.
-
-
-
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49
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14344278292
-
-
note
-
With R = n-Pr, β-H transfer to Zr (starting from conformation D in Figure 11) is found to have an energy barrier of 116 kJ/mol, whereas β-H transfer to a coordinated monomer (starting from conformation B) has a barrier of 23 kJ/mol. The corresponding termination barriers with R = H are 146 and 34 kJ/mol, respectively.
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-
-
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50
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14344273241
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note
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Chain transfer to TMA or MAO results in saturated end groups. When this mechanism is dominating, it is reflected in large deviations between the FTIR- and GPC-determined molecular weights.
-
-
-
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51
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14344284319
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note
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6 and is estimated to be in the range 60-80 kJ/mol from DFT reaction pathway calculations (increasing the Hβ-Cβ distance).
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